Zoom optical system

ABSTRACT

An optical system composed, in order from the object side, of a first lens unit which has a positive power or is powerless, a second lens unit which has a positive power, a third lens unit which has a positive power and a fourth lens unit which has a negative power, and configured to change its magnification by varying airspaces reserved between the lens unit. The fourth lens unit is composed of a single lens element or the optical system as a whole is composed of lens element in a number not exceeding twice a number of movable lens units. The optical system is composed of a small number of lens elements and compact.

This is a continuation-in-part of U.S. patent application Ser. No. 09/365,246, filed on Jul. 30, 1999, now abandoned, which is a division of U.S. patent application Ser. No. 09/014,386, filed on Jan. 27, 1998, now U.S. Pat. No. 6,014,2655.

BACKGROUND OF THE INVENTION

a) Field of the Invention

The present invention relates to a zoom optical system which is to be used with photographic cameras, and lens shutter cameras in particular.

b) Description of the Prior Art

In the recent years, lens shutter cameras which are equipped with zoom optical systems are configured as the so-called collapsible mount type which accommodate lens systems into camera bodies by narrowing airspaces between adjacent lens units of the optical systems. For reducing thickness of a lens shutter camera, it is therefore necessary to shorten a total length of an optical system in its collapsed condition. Further, a zoom optical system has a long total length at its tele position, and it is necessary to configure a lens barrel which accommodates and holds a lens system so that it can be accommodated in two or more stages in a camera body for collapsing the optical system compact at its tele position, thereby reducing thickness of the camera.

A typical zoom optical system which is conventionally used in lens shutter cameras is composed of three positive, positive and negative lens units for obtaining a relatively high vari-focal ratio and a compact design.

For obtaining a wide field angle of incidence at a wide position of such a zoom optical system which is composed of the three positive, positive and negative lens units, a total refractive power of the first positive lens unit and the second positive lens unit must be strengthened at the wide position, and the second lens unit must be composed of a large number of lens elements for favorably correcting offaxial aberrations in the second lens unit in particular.

For maintaining favorable optical performance in all zoom regions from a wide position to a tele position, it is necessary to suppress amounts of aberrations to be produced in each zoom lens unit. Since the third lens unit produces aberrations in large amounts at the tele position in particular, it is necessary for reducing the aberrations to use two or more lens elements in the third lens unit.

Let us suppose that we are to obtain a zoom optical system which is composed of three positive, positive and negative lens units, covers a region wherein field angles are large and has a vari-focal ratio of 3 or higher. When a lens barrel is composed of two or three stages for collapsing the zoom optical system which has a long total length at its tele position and moves the first lens unit for a long distance, a single stage of the lens barrel is longer than a total length of the optical system in which airspaces between adjacent lens units are narrowed, thereby making it difficult to reduce thickness of a camera. When the lens barrel is composed of four or more stages, the lens barrel has a large maximum diameter which is disadvantageous for compact configuration of a camera.

As conventional examples which are configured for correcting the defects described above, there are known zoom optical systems disclosed by Japanese Patents Kokai Publication No. Hei 6-214157 and Kokai Publication No. Hei 6-214158 each of which comprises four positive, positive, positive and negative lens units movable at magnification change stages for obtaining a vari-focal ratio of 3 or higher and a compact design, and is configured to reduce aberrations to be produced by changing the magnification, zoom optical systems disclosed by Japanese Patents Kokai Publication No. Hei 8-122640 and Kokai Publication No. Hei 9-101457 each of which is composed of four positive, negative, positive and negative lens units, and zoom optical systems disclosed by Japanese Patents Kokai Publication No. Hei 9-15499 and No. Hei 9-15500 each of which is composed of four negative, positive, positive and negative lens units.

In each of the optical systems disclosed by Japanese Patents Kokai Publication No. Hei 6-214157, No. Hei 6-214158, No. 8-122640 and No. Hei 9-101457 out of the conventional examples mentioned above, the fourth lens unit is composed of two or more lens elements and has a composition wherein a lens element or lens elements are disposed on the object side of a negative lens element which has a deep concave surface on the object side and is disposed on the image side. Accordingly, an axial distance as measured from a surface of incidence to a surface of emergence of the fourth lens unit, i.e., compositional length of the fourth lens unit is long and inadequate for shortening a compositional length of a lens barrel in its collapsed condition. That is, the optical system has a composition such as that shown in FIG. 1 and is not preferable for shortening a compositional length of a lens barrel in its collapsed condition. In FIG. 1, reference symbols G1, G2, G3 and G4 represent the first, second, third and fourth lens units, a reference symbol S designates an aperture stop, and reference symbols L_(P) and L_(N) denote a positive lens element and a negative lens element.

Further, the optical system disclosed by Japanese Patent Kokai Publication No. Hei 9-15499 has a field angle of incidence 2ω not narrower than 65° but a low vari-focal ratio on the order of 2.9. Furthermore, the optical system disclosed by Japanese Patent Kokai Publication No. Hei 9-15500 has a field angle of incidence 2ω not narrower than 65° and a vari-focal ratio on the order of 3.8, but allows an aperture stop to move at a magnification change stage, whereby the optical system comprises a large number of parts which are moved for changing a magnification, uses a lens barrel having a complicated structure or a large number of parts and requires a high manufacturing cost.

Moreover, each of the optical systems disclosed by Japanese Patents Kokai Publication No. Hei 9-15499 and No. 9-15500 is a zoom optical system composed of the four negative, positive, positive and negative lens units which are composed of lens elements in a relatively small number of seven, but uses a front lens element having a large diameter due to a fact that an aperture stop is disposed in the second lens unit which is disposed with a relatively wide airspace from the first lens unit. Since this optical system is focused onto an object located at a short distance by moving the third lens unit toward the object side, this optical system remarkably aggravates spherical aberration at its tele position in particular and hardly allows to shorten the distance to the object. Spherical aberration is remarkably aggravated since a converging light bundle which has passed through the second positive lens unit is incident onto the third lens unit and rays pass through high portions of a first negative lens element of the third lens unit in a condition where the third lens unit is moved toward the object side for focusing, and this aggravation is more remarkable at the tele position in particular.

In addition, it is strongly demanded to configure cameras more compact and problems are posed to dispose relatively large areas of lens surfaces which are disposed near a film surface and through which effective rays do not pass.

SUMMARY OF THE INVENTION

A primary object of the present invention is to provide a compact zoom optical system which has a high vari-focal ratio, is composed of a small number of lens elements and permits shortening a length of a lens barrel in its collapsed condition.

Another object of the present invention is to provide a zoom optical system which permits reducing diameters of a front lens element and a stop.

Still another object of the present invention is to provide a zoom optical system which is composed of a small number of lens elements and allows aberrations to be varied little when the optical system is focused onto an object located at an extremely short distance.

The zoom optical system according to the present invention which has a first composition is composed, in order from the object side, of a first lens unit which has a positive power or is powerless (having substantially no refractive power), a second lens unit which has a positive power, a third lens unit which has a positive power and a fourth lens unit which has a negative power, configured to change a magnification by-varying-airspaces reserved between the lens units, and characterized in that the fourth lens unit is composed of a single lens element.

Further, the zoom optical system according to the present invention which has the first composition described above is characterized in that it satisfies the following condition (8):

0≦y/f ₁≦0.14  (8)

The zoom optical system according to the present invention which has a second composition is composed, in order from the object side, of a first lens unit which has a positive power or is powerless, a second lens unit which has a positive power, a third lens unit which has a positive power and a fourth lens unit which has a negative power, configured to change a magnification by changing airspaces reserved between the lens units, and characterized in that the optical system satisfies the following condition (1);

0.03<ΣD ₄ /y<0.25  (1)

The zoom optical system according to the present invention which has a fourth composition is composed, in order from the object side, of a first lens unit which has a positive power or is powerless, a second lens unit which has a positive power, a third lens unit which has a positive power and a fourth lens unit which has a negative power, configured to change a magnification by changing airspace reserved between the lens units, and characterized in that the fourth lens unit is composed of a single lens element, and that an aperture stop is disposed on the image side of a first lens element of the second lens unit and on the object side of the third lens unit.

The zoom optical system according to the present invention which has a fifth composition has the fourth composition and is characterized in that it satisfies the following condition (10):

0.10≦E(W)/f _(W)≦0.30  (10)

The zoom optical system according to the present invention which has a sixth composition is composed of a first lens unit which has a positive power or is powerless, a second lens unit which has a positive power, a third lens unit which has a positive power and a fourth lens unit which has a negative power, configured to change a magnification by changing airspaces reserved between the lens units, and is characterized in that an aperture stop is disposed between the second lens unit and the third lens unit and that the aperture stop is moved together with the second lens unit or toward the object side independently of movements of the other lens units for changing a magnification from a wide position to a tele position.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a conceptional diagram of a conventional optical system;

FIG. 2 shows a conceptional diagram of the optical system according to the present invention;

FIGS. 3A and 3B show diagrams illustrating relationship between an effective portion and a shape of a lens element;

FIGS. 4 through 22 show sectional views illustrating compositions of first through nineteenth embodiments of the optical system according to the present invention; and

FIGS. 23A, 23B and 23C show diagrams illustrating conditions of rays which are refracted by cemented lens components.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

The zoom optical system according to the present invention which has a first composition is composed, in order from the object side, of a first lens unit which has a positive refractive power or is powerless, a second lens unit which has a positive refractive power, a third lens unit which has a positive refractive power and a fourth lens unit which has a negative refractive power, configured to change a magnification by changing airspaces reserved between the lens units, and characterized in that the fourth lens unit is composed of a single lens element.

The zoom optical system according to the present invention is configured to change the magnification by changing the airspaces reserved between the lens units as described above. A magnification is changed from a wide position to a tele position, for example, by moving the first lens unit and the fourth lens unit toward the object side, and then moving the second lens unit and the third lens unit toward the object side later. Speaking more concretely, the magnification is changed from the wide position to the tele position by moving all the lens units toward the object side (changing the airspaces between the lens units) so as to widen an airspace reserved between the first lens unit and the second lens unit, and narrow an airspace reserved between the third lens unit and the fourth lens unit. Further, an airspace reserved between the second lens unit and the third lens unit is changed so that aberrations such as spherical aberration, curvature of field and chromatic aberrations are varied little by changing the magnification.

The zoom optical system according to the present invention allows the fourth lens unit to have a short compositional length and permits shortening a compositional length of a lens barrel in its collapsed condition since it is composed of the four positive, positive, positive and negative lens units, and characterized in that the fourth lens unit is composed of the single lens element as described above.

There is known a zoom lens system which is composed of four lens units as described above and uses a negative lens element having a deep concave surface on the object side and disposed on the image side (on the image side in a fourth lens unit) as in the conventional example described above. The present invention also uses a negative lens element which has a deep concave surface on the object side as in embodiments described later. When the fourth lens unit is composed of a negative lens element which has a deep concave surface on the object side, the third lens unit can fit into this surface in the collapsed condition, thereby making it possible to further shorten a compositional length of a lens barrel in its collapsed condition.

FIGS. 1 and 2 compare the conventional example described above with the optical system according to the present invention. A composition of the conventional zoom lens system and a composition of the optical system according to the present invention are shown in FIG. 1 and FIG. 2 respectively wherein a reference symbol W represents a wide position and a reference symbol C designates a collapsed condition. As seen from these drawings, a lens element L, is disposed on the object side of an object side concave surface of a negative lens element L_(n) in the fourth lens unit and a portion of a third lens unit G3 does not fit into a fourth lens unit G4. In the zoom optical system according to the present invention, in contrast, a fourth lens unit G4 is composed of a single lens element L_(n) which has a deep concave surface on the object side and a portion of a third lens unit G3 penetrates into this deep concave surface. Accordingly, the zoom optical system according to the present invention makes it possible to further shorten a lens barrel structure in its collapsed condition. Speaking concretely, the zoom optical system according to the present invention in which the fourth lens unit G4 is composed of the single negative lens element L_(n) having the deep concave surface on the object side can be shorter for a distance corresponding to a difference between a first surface A of the conventional zoom optical system in its collapsed condition (a first surface A in the collapsed condition shown at an upper stage C in FIG. 1) and a first surface B of the zoom optical system according to the present invention in its collapsed condition shown in FIG. 2.

Further, the zoom optical system according to the present invention which has the first composition described above is characterized in that it satisfies the following condition (8):

0≦y/f ₁≦0.14  (8)

wherein the reference symbol y represents ½ of a diagonal length of an image surface and the reference symbol f1 designates a focal length of the first lens unit.

The condition (8) defines a refractive power of the first lens unit and is adopted for reducing variations of aberrations to be caused by changing a magnification. If the upper limit of 0.14 of the condition (8) is exceeded, the first lens unit will have a strong refractive power, thereby making it difficult to correct astigmatism and coma favorably in the vicinities of the tele position. If the lower limit of 0 of the condition (8) is exceeded, in contrast, the first lens unit will have a negative refractive power, the first lens unit and the second lens unit will compose a retrofocus type lens system which has a long back focal length, the zoom optical system will have a large total length at the wide position, and a wide airspace is reserved between the first lens unit and the second lens unit, whereby the first lens unit will have a large diameter and it will be impossible to configure a lens barrel compact. Further, it will be difficult to correct spherical aberration favorably at the tele position in particular.

A second composition of the zoom optical system according to the present invention is described below. Like the zoom optical system which has the first composition described above, the zoom optical system according to the present invention which has the second composition is composed, in order from the object side, of a first lens unit which has a positive refractive power or is powerless, a second lens unit which has a positive refractive power, a third lens unit which has a positive refractive power and a fourth lens unit which has a negative refractive power, configured to change a magnification by varying airspaces reserved between the lens units, and characterized in that the zoom optical system satisfies the following condition (1):

0.03<ΣD ₄ /y<0.25  (1)

wherein the reference symbol ΣD₄ represents a structural length of the fourth lens: unit, i.e., a distance on an optical axis as measured from a surface of incidence to a surface of emergence of the fourth lens unit and the reference symbol y designates ½ of a diagonal length of an image surface.

The zoom optical system according to the present invention which has the second composition described above is configured to satisfy the condition (1) for shortening a structural length of a lens barrel in its collapsed condition.

If the upper limit of 0.25 of the condition (1) is exceeded, the third lens cannot penetrate into the fourth lens unit, thereby prolonging a structural length of lens barrel in its collapsed condition.

If a lower limit of 0.03 of the condition (1) is exceeded, the fourth lens unit will have a small structural length which is advantageous for thinning a camera but the lens element of the fourth lens unit will be too thin for practical working.

Though the fourth lens unit which is composed of a single lens element is not limitative for the zoom optical system according to the present invention, it is desirable that the condition (1) is satisfied even when the fourth lens unit is composed of a single lens element as in the first embodiment.

The zoom optical system according to the present invention which has a third composition is composed, in order from the object side, of a first lens unit having a positive refractive power or is powerless, a second lens unit having a positive refractive power, a third lens unit having a positive refractive power and a fourth lens unit having a negative refractive power, configured to change a magnification by varying airspaces reserved between the lens units, and characterized in that the optical system is composed of lens elements in a number not exceeding twice a number of lens units which are movable for changing the magnification.

Since the optical system according to the present invention is a zoom optical system composed of four lens units, the zoom optical system according to the present invention which has the third composition is characterized in that it is composed of lens elements in a number of eight or smaller.

It is desirable that the zoom optical system according to the present invention which has the third composition is composed of lens elements in a number of seven or smaller.

Further, it is desirable that the zoom optical system according to the present invention which has the third composition is composed of lens elements in a number of six or smaller.

When the zoom optical system as a whole is composed of a small number of lens elements, the optical system is compact as a whole and each lens unit is composed of a small number of lens element or elements, whereby each lens unit can have a short structural length and a lens barrel can have a short structural length in its collapsed condition.

It is desirable for the zoom optical system which has the first, second or third composition that the fourth lens unit satisfies the following condition (2):

−1.20<(r _(F) +r _(R))/(r _(F) −r _(R))<0  (2)

wherein the reference symbols r_(F) and r_(R) represent radii of curvature on an object side surface and an image side surface respectively of the fourth lens unit.

If the upper limit of 0 of the condition (2) is exceeded, a final surface of the optical system (the image side surface of the fourth lens unit) will be deep, or has strong curvature, whereby an edge of a final lens element becomes nearer a film surface and a distance as measured from a first surface to the final surface of the lens system is substantially prolonged. If the lower limit of −1.20 of the condition (2) is exceeded, in contrast, a surface of incidence of a final lens unit (an object side surface of the fourth lens unit) will have strong curvature or a too deep a concave shape and interfere with a barrel member disposed on the object side of this surface, thereby making it necessary to widen an airspace reserved between the lens units.

It is desirable for the zoom optical system which has the first, second or third composition described above that at least one aspherical surface is disposed at least on the fourth lens unit.

Since a magnification of a zoom optical system which is composed of four positive, positive, positive and negative lens units is changed mainly by the fourth lens unit, it is effective for shortening a total length of the lens system to strengthen the negative refractive power of the fourth lens unit. Accordingly, a lens element disposed in the fourth lens unit has strong curvature and aggravates aberrations such as curvature of field and distortion of marginal rays. This aggravation of aberrations can be prevented or the aberrations of the marginal rays can be corrected favorably by configuring at least one of the surfaces of the fourth lens unit as an aspherical surface which has curvature moderated at a marginal portion.

In the zoom optical system according to the present invention which has the first, second or third composition, chromatic aberration is not corrected independently in each lens unit but cancelled each other among the lens units so as to be small in the optical system as a whole. This design concept allows the aberration (chromatic aberration) to remain in each lens unit, thereby making it possible to compose each lens unit of a small number of lens elements or compose the optical system as a whole of seven or a smaller number of lens elements.

When the fourth lens unit which has the strong refractive power is composed of a single negative lens element in particular, the fourth lens unit produces chromatic aberration in a large amount, thereby making it difficult to cancel it with chromatic aberration produced by the lens units disposed before the fourth lens unit. For this reason, it is desirable to configure the fourth lens unit so as to satisfy the following condition (3):

ν_(R)>50  (3)

wherein the reference symbol ν_(R) represents an Abbe's number of the negative lens element of the fourth lens unit.

If the lower limit of 50 of the condition (3) is exceeded, the fourth lens unit will produce chromatic aberration in an amount too large for sufficient correction with the lens units disposed before the fourth lens unit.

For the zoom optical system according to the present invention, it is desirable to dispose an aperture stop on the object side of a final lens element of the third lens unit. For shortening a structural length of a lens barrel in its collapsed condition, it is desirable to penetrate the third lens unit into the object side concave surface of the fourth lens unit as described above. When an aperture stop is disposed on the image side of the third lens unit, the aperture stop interferes with a marginal portion of the fourth lens unit, thereby prolonging a length in the collapsed condition.

Further, it is desirable to configure the zoom optical system according to the present invention so as to satisfy the following conditions (4) and (5):

1.5<β_(4T)/β_(4W)  (4)

0.1<f _(BW) /f _(W)<0.5  (5)

wherein the reference symbols β_(4T) and β_(4W) represent lateral magnifications of the fourth lens unit at a tele position and a wide position respectively, the reference symbol f_(BW) designates a back focal length at the wide position, and the reference symbol f_(W) denotes a focal length of the optical system as a whole at the wide position.

The condition (4) is required for obtaining a high vari-focal ratio of the zoom optical system according to the present invention. If the lower limit of 1.5 of the condition (4) is exceeded, a burden for the magnification change shifts from the fourth lens unit to the third lens unit and each lens unit is moved for a longer distance to change the magnification, thereby making it impossible to shorten the optical system in the thrust direction.

The condition (5) is required for shortening diameters of the lens elements. If the lower limit of 0.1 of the condition (5) is exceeded, the fourth lens unit will be too near the film surface and lens elements will have too large diameters. If the upper limit of 0.5 of the condition (5) is exceeded, the lens element will have small diameters but the fourth lens unit will have too high a lateral magnification, thereby making it impossible to correct aberrations favorably.

Furthermore, it is desirable for the zoom optical system according to the present invention that the fourth lens unit satisfies the following condition (6):

0.5<|f ₄ /f _(W)|<0.9  (6)

wherein the reference symbol f₄ represents a focal length of the fourth lens unit.

If the lower limit of 0.5 of the condition (6) is exceeded, the fourth lens unit will have too strong a refractive power, thereby making it impossible to correct aberrations favorably. If the upper limit of 0.9 of the condition (6) is exceeded, in contrast, the lens system will have a large total length, thereby making it impossible to configure the zoom optical system compact.

For reducing variations of aberrations to be caused by focusing the zoom optical system according to the present invention, it is desirable to focus the optical system by moving the third lens unit. In addition, it is possible to focus the optical system by moving the second lens unit or the fourth lens unit, the second lens unit together with the third lens unit or the optical system as a whole.

When the zoom optical system is to be focused by moving the third lens unit, it is desirable to configure the third lens unit so as to satisfy the following condition (7):

|β_(3T)|<0.9  (7)

wherein the reference symbol β_(3T) represents a magnification of the third lens unit at the tele position.

If the upper limit of 0.9 of the condition (7) is exceeded, the third lens unit must be moved for a long distance for focusing the optical system.

It is more desirable that the optical system which has the composition described above satisfies the following condition (9):

0.5<|f ₄ |/y<1.0  (9)

wherein the reference symbol f₄ represents a focal length of the fourth lens unit.

The zoom optical system according to the present invention is composed as described above so that variations of aberrations caused by a magnification change are shared among the lens units, whereby aberrations are corrected favorably in the optical system as a whole and favorable optical performance is maintained even when the lens units consist of a reduced number of lens elements.

That is, the zoom optical system according to the present invention is composed of four lens units as exemplified by a ninth embodiment described later and configured to change its magnification by moving the lens units and minimize a burden on the first lens unit at a stage of a magnification change performed by moving the lens units, whereby the first lens unit shares correction of aberrations, astigmatism and coma in particular, caused due to movements of the second lens unit and the third lens unit of the optical system according to the present invention which correspond to the first lens unit and the second lens unit of the conventional zoom lens system which is composed of three positive, positive and negative lens units. Accordingly, this composition lessens a burden on each lens unit for correction of aberrations even when the zoom optical system has a high vari-focal ratio of 3.5 or higher, thereby making it possible to compose the zoom optical system of lens elements in a number smaller than that of the lens elements of the conventional zoom lens system composed of the three lens units. Further, the zoom optical system according to the present invention which has the composition described above is capable of favorably correcting aberrations only with the first through third lens units, thereby lessening a burden on the fourth lens unit for the correction of aberrations and permitting enhancing a power of the fourth lens unit. Accordingly, the zoom optical system according to the present invention can have a short back focal length and a total length shorter than that of the conventional zoom lens system which is composed of four lens units.

Since the composition lessens the burden on the fourth lens unit for the correction of aberrations, it makes it possible to compose the fourth lens unit of a single negative lens element. When the fourth lens unit is composed of a single negative lens element, the negative lens element used as the fourth lens unit has a surface of incidence which is a rather deep concave surface into which the third lens unit can penetrate in a collapsed condition as shown in FIG. 2, thereby making it possible to shorten a length of a lens barrel in its collapsed condition.

The condition (9) defines a refractive power of the fourth lens unit, and is required for obtaining a field angle of incidence of 65° or larger at the wide position and favorable optical performance. If the lower limit of 0.5 of the condition (9) is exceeded, the fourth lens unit will have a strong refractive power which is advantageous for obtaining a field angle of incidence of 65° or larger at the wide position but makes it difficult to correct aberrations favorably. If the upper limit of 1.0 of the condition (9) is exceeded, in contrast, the fourth lens unit will have a weak refractive power which makes it difficult to correct aberrations favorably when the zoom optical system has a wide field angle.

It is desirable for the zoom optical system according to the present invention to dispose an aperture stop on the object side of an image side lens element of the third lens unit.

It is desirable to configure the object side surface of the negative lens element of the fourth lens unit as a deep concave surface as described above so that the third lens unit penetrates into the concave surface in a collapsed condition. When an aperture stop is disposed on the image side of the third lens unit, however, the aperture stop will interfere with a marginal portion of the fourth lens unit, thereby undesirably prolonging a total length in the collapsed condition.

Further, it is desirable to dispose an aperture stop between the second lens unit and the third lens unit, and move the aperture stop together with the second lens unit for changing a magnification. By disposing an aperture stop between the second lens unit and the third lens unit, and moving it together with the second lens unit as described above, it is possible to reduce the variations of aberrations to be caused by changing a magnification from the wide position to the tele position and obtain favorable optical performance of the zoom optical system as a whole. Further, it is possible to bring an entrance pupil close to the first lens unit at the tele position, thereby lowering offaxial rays passing through the first lens unit and the second lens unit. Accordingly, it is possible to reduce diameters of the first lens unit and the second lens unit, thereby configuring a lens barrel compact.

For the zoom optical system according to the present invention which has one of the compositions described above, it is desirable to use at least one aspherical surface in the fourth lens unit.

A magnification of the zoom optical system according to the present invention is changed mainly by the fourth lens unit. To use the zoom optical system in a condition where it has a short total length, it is therefore effective to strengthen the negative refractive power of the fourth lens unit. When the negative refractive power of the fourth lens unit is strengthened, however, a lens element used as the fourth lens unit has strong curvature which aggravates offaxial aberrations such as astigmatism and distortion. To correct these aberrations, it is desirable to configure at least one surface as an aspherical surface having such a shape as to lower curvature toward marginal portions. Such an aspherical surface makes it possible to correct the offaxial aberrations favorably.

For the zoom optical system according to the present invention, it is desirable to use at least one aspherical surface on a positive lens element disposed in the third lens unit. When a field angle of incidence is enlarged at the tele position in particular, offaxial rays passing through the third lens unit produce remarkable aberrations, astigmatism and coma in particular. For this reason, it is desirable to configure at least one surface of the positive lens element as an aspherical surface. Such an aspherical surface makes it possible to correct the aberrations produced by the offaxial rays.

The zoom optical system according to the present invention is composed of lens elements in a number not exceeding twice the number of the lens units which are moved for changing a magnification as described above. To correct chromatic aberration favorably in the zoom optical system according to the present invention which has the composition described above, it is desirable to correct chromatic aberration not in each lens unit independently but to cancel chromatic aberration among the'lens units so that it is corrected favorably in the zoom optical system as a whole. This design concept allows chromatic aberration to remain in each lens unit, thereby making it possible to compose the zoom optical system as a whole of lens elements in a number not exceeding twice the number of the lens unit which are moved for zooming from the wide position to the tele position, shorten a structural length of each lens unit and shorten a length of a lens barrel in its collapsed condition.

Speaking concretely of longitudinal chromatic aberration, it is produced remarkably by the second lens unit and aggravated toward the tele position. Therefore, the longitudinal chromatic aberration can be cancelled by producing chromatic aberration in a reverse direction by the first lens unit and the fourth lens unit.

Lateral chromatic aberration is produced remarkably by the first lens unit and the fourth lens unit, and aggravated toward the tele position. The chromatic aberration can be cancelled by configuring the third lens unit so as to produce chromatic aberration reverse to that produced by the first lens unit and configuring the second lens unit so as to produce chromatic aberration reverse to that produced by the fourth lens unit. Accordingly, chromatic aberration can be corrected favorably in the zoom optical system as a whole even when chromatic aberration is. produced in a large amount by each lens unit which is composed of a small number of lens elements.

For the zoom optical system according to the present invention, it is desirable to compose the second lens unit of a positive meniscus lens element which has a convex surface on the object side. To obtain favorable optical performance of the zoom optical system as a whole in which the second lens unit is composed of a single positive lens element, it is desirable to configure the lens element as a positive meniscus lens element which has a convex surface on the object side.

When the fourth lens unit which has the strong refractive power is composed of a single negative lens element, the fourth lens unit produces chromatic aberration in a large amount and it is difficult to correct the chromatic aberration with the lens units disposed on the object side of the fourth lens unit. For this reason, it is desirable to configure the negative lens element used as the fourth lens unit so as to satisfy the condition (3) mentioned above.

It is desirable that the zoom optical system according to the present invention which has one of the compositions described above is focused on an object located at a short distance by moving the third lens unit toward the object side. By focusing the zoom optical system as described above, it is possible to reduce the variations of aberrations to be caused by focusing.

Further, the variations of aberrations to be caused by changing a magnification can easily be reduced by configuring the first lens unit so as to be more powerless or satisfy, in place of the condition (8), the following condition (8-1):

0<y/f ₁<0.07  (8-1)

When a refractive power of the first lens unit is defined so as to satisfy the condition (8) or the condition 8-1), it is desirable to compose the first lens unit of a negative lens element and a positive lens element in order from the object side.

Furthermore, it is desirable that the zoom optical system according to the present invention which has one of the compositions described above satisfies the following condition (4-1):

1.5<β_(4T)/β_(4W)<6.0  (4-1)

The condition (4-1) defines an upper limit of the condition (4) so as to further restrict the condition (4). If the upper limit of 6.0 of the condition (4-1) is exceeded, a burden on the fourth lens unit for a magnification change at the tele position will be heavier, thereby making it difficult to obtain favorable optical performance of the zoom optical system as a whole.

Moreover, it is desirable that the zoom optical system according to the present invention which has one of the compositions described above satisfies the condition (5) mentioned above.

When the zoom optical system is focused by moving the third lens unit, it is desirable to satisfy the condition (7) mentioned above:

The zoom optical system according to the present invention which has a fourth composition is composed of a first lens unit which has a positive power or is powerless, a second lens unit which has a positive power, a third lens unit which has a positive power and a fourth lens unit which has a negative power, and characterized in that the fourth lens unit is composed of a lens component (a lens element or a cemented lens component) which has a concave surface on the object side, and that an aperture stop is disposed on the image side of a lens component disposed on the object side in the second lens unit and on the object side of the third lens unit.

When a fourth lens unit is composed of a single lens component which has a concave surface on the object side as in the zoom optical system according to the present invention described above, a third lens unit can penetrate into the fourth lens unit in a collapsed condition as shown in FIG. 2. The fourth lens unit can have thickness which is smaller than a total of thickness and an airspace of a lens unit which is composed of two or more lens elements disposed with an airspace reserved, thereby allowing a third lens unit to be brought closer to a film surface and exhibiting a higher effect of the collapsible mount.

Further, the zoom optical system according to the invention in which the fourth lens unit is composed of a single lens component, and the aperture stop is disposed on the image side of the lens component disposed on the object side in the second lens unit and on the object side of the third lens unit is capable of correcting lateral chromatic aberration, etc. produced by the fourth lens unit and aberrations of paraxial rays with good balance by a small number of lens elements. When the aperture stop is disposed on the image side of the lens component disposed on the object side in the second lens unit, paraxial rays are adequately separated from offaxial rays in the first lens unit and a light bundle passing through the fourth lens unit does not occupy too large a region, whereby it is possible to correct lateral chromatic aberration, etc. produced by the fourth lens unit and aberrations of the paraxial rays with a small number of lens elements. When the aperture stop is disposed on the object side of the third lens unit, the first lens unit does not require too large a diameter, at least one lens element of the second lens unit is disposed before the aperture stop and the third lens unit is disposed after the aperture stop, whereby it is possible to reduce the variations of spherical aberration, curvature of field, chromatic aberration, etc. to be caused mainly by a magnification change with a small number of lens elements.

In the zoom optical system according to the present invention which has the fourth composition, the cemented lens component which is composed only of an aspherical glass lens element having a meniscus shape and a spherical lens element may be disposed not in a rear lens group, but in a front lens group or each of the front lens group and the rear lens group.

In other words, the zoom optical system according to the present invention which has the fourth composition comprises a positive front lens group which consists of one movable lens unit or a plurality of movable lens units and a negative rear lens group, and at least one cemented lens component which consists only of an aspherical glass lens element having a meniscus shape and a spherical lens element.

Furthermore, the zoom optical system according to the present invention which has a fifth composition comprises a lens group which comprises a single or a plurality of movable lens units and has a positive power, and a lens group which has a negative power: at least one of lens components disposed in the lens group having the negative power being a cemented lens component which is composed only of an aspherical glass lens element having a meniscus shape and a spherical lens element.

The zoom optical system according to the present invention which has the fifth composition comprises the lens group having the positive power and the lens group having the negative power in order from the object side or the lens group having the negative power and the lens group having the positive power in the order from the object side.

For the zoom optical system according to the present invention which has the fourth composition, it is desirable that the front lens group comprises, in order from the object side, a first lens unit, second lens unit and a third lens unit, that the rear lens group consists only of a fourth lens unit, and that the optical system moves the first lens unit, the second lens unit and the third lens unit to change a magnification.

Furthermore, it is desirable that the zoom optical system which comprises the front lens group comprising the first through third lens units and the rear lens group, and moves the first through third lens units to change the magnification is configured to satisfy any one of the conditions (1), (2), (3), (4-1), (6), (7), (8) and (11). Furthermore, the zoom optical system may be configured to satisfy a plurality or all of these conditions.

The zoom optical system according to the present invention which has the fourth composition may be configured so that the front lens group having the positive refractive power comprises a first lens unit and a second lens unit, the first lens unit and the second lens unit are moved to change a magnification, and at least a negative lens component of the rear lens unit is configured as a cemented lens component which consists only of an aspherical glass lens element having a meniscus shape and a spherical lens element. That is, the zoom optical system described above is a lens system comprising the front lens group having the positive refractive power and the rear lens group having the negative refractive power, wherein the front lens group comprises a first lens unit and a second lens unit, at least a negative lens component disposed in the rear lens group having the negative refractive power is a cemented lens component which consists only of an aspherical glass lens element having a meniscus shape and a spherical lens element, and the first lens unit and the second lens unit of the front lens group are moved to change a magnification.

It is preferable that this zoom optical system satisfies at lest either of the conditions (8) and (11).

It is desirable to configure the zoom optical system according to the present invention which has the fourth composition so that the positive front lens group comprises a first lens unit and a second lens unit, the first and the second lens unit are moved to change a magnification, and at least one lens component disposed in the zoom optical system is a cemented lens component which consists only of an aspherical glass lens element having a meniscus shape and a spherical lens element.

It is desirable that the zoom optical system described above satisfies at least either of the abovementioned conditions (8) and (11).

It is desirable that each of the zoom optical systems which have the fourth and fifth compositions described above satisfies at least one of the conditions (5) through (10).

To compose a cemented lens component which is to be used in the zoom optical system according to the present invention by cementing an aspherical glass lens element to a spherical glass lens element, it is preferable to smooth an aspherical surface of the aspherical glass lens element which is to be kept in contact with air and leave a surface of the lens element which is to be cemented as it is a rough surface.

A surface of a lens element which is to be used in a cemented lens component is to be cemented to another lens element with a cementing agent or the like. Lens elements which are to be disposed before and after a cemented surface are made of, materials having refractive indices which are different from each other so that the cemented lens component correct chromatic aberration and other aberrations. However, it is not necessary to reserve a large difference between the refractive indices when a difference is reserved between Abbe's numbers as required to correct chromatic aberration.

Even when surfaces of two lens element which are to be cemented to each other are somewhat rough, it is possible to allow a design refracted condition of rays to remain substantially unchanged and not to degrade an image quality so much by selecting a cementing agent which has a refractive index close to those of two lens elements to be cemented to each other since a cementing agent is filled between the lens elements disposed before and after a cemented surface of a cemented lens component.

When surfaces of a cemented lens component are kept in contact with air are rough, on the other hand, these rough surfaces make a refracted condition of rays different from that assumed at a designated stage, therby degrading an image quality.

By configuring the aspherical lens element to be used in the zoom optical system according to the present invention so as to have a smooth surface which is to be kept in contact with air and a rough surface which is to be cemented as described above, it is possible to manufacture at a low cost a cemented lens component which allows a refracted condition of rays to remain substantially unchanged from that assumed at the design stage, thereby obtaining a vari-focal optical system which scarcely degrades an image quality.

Refracted conditions of rays will be described taking as an example cemented lens components which are to be used in a fourth lens unit G4 of an optical system preferred as a nineteenth embodiment illustrated in FIG. 22.

FIGS. 23A, 23B and 23C show diagrams illustrating cemented lens components to be used in the fourth lens G4 of the nineteenth embodiment and conditions of rays refracted by these cemented lens components. Out of these drawings, FIG. 23A shows a condition of rays refracted by a cemented lens component using a lens element having two surfaces which are worked smooth so as to have design values, FIG. 23B shows a condition of rays refracted by a cemented lens component using a lens element having an air contact surface which is worked smooth as it is designed and a rough surface to be cemented, and FIG. 23C shows a condition of rays refracted by a cemented lens component using a lens element having a rough air contact surface and a rough surface to be cemented which is worked smooth as it is designed.

As apparent from these drawings, the cemented lens component shown in FIG. 23B provides a condition of refracted rays which is substantially unchanged from that obtained with the cemented lens component shown in FIG. 23A, whereas the cemented lens component shown in FIG. 23C provides a condition of refracted rays which is different from that obtained with the cemented lens component shown in FIG. 23A.

The cemented lens component shown in FIG. 23B which is manufactured as described above allows an influence due to the rough cemented surface to be almost cancelled by a cementing agent which has a refractive index close to those of two lens elements of the cemented lens component, thereby providing the condition of refracted rays which remains substantially unchanged from that assumed at the design stage. On the other hand, the cemented lens component shown in FIG. 23C which has the rough air contact surface provides the condition of refracted rays which is different from that assumed at the design stage.

Then, the zoom optical system according to the present invention which has a fifth composition is composed, in order from the object side, of a first lens unit which has a positive power or is powerless, a second lens unit which has a positive power, a third lens unit which has a positive power and a fourth lens unit which has a negative power, and is characterized in that an aperture stop is disposed between a lens element disposed on the object side in the second lens unit and an object side surface of the third lens unit, and that the zoom optical system satisfies the following condition (10):

0.10≦E(W)/fw≦0.30  (10)

wherein the reference symbol E (W) represents a distance as measured from a vertex of a first surface of the zoom optical system at a wide position to an entrance pupil and the reference symbol fw designates a focal length of the zoom optical system as a whole at the wide position.

If the upper limit of 0.30 of the condition (10) is exceeded, a diameter of a front lens element of the zoom optical system will be enlarged contrary to the object of compact configuration of cameras, and adverse influences will be produced on layout and design of cameras. If the lower limit of 0.10 of the condition (10) is exceeded, in contrast, aberrations of marginal rays will be aggravated and a diameter of a rear lens element will be enlarged.

To further reduce a diameter of a front lens element, it is desirable to satisfy, in place of the condition (10), the following condition (10-1):

0.10≦E(W)/fw23 0.24  (10-1)

When the zoom optical system according to the present invention which has the fifth composition is configured to be zoomed by moving the aperture stop together with the second lens unit, an airspace between the second lens unit and the aperture stop can be narrowed so as to obtain a mechanical advantage.

It is desirable that the zoom optical system according to the present invention which has the fourth or fifth composition is focused-by an object located at a short distance by moving the second lens unit and the third lens unit toward the object side.

That is, the zoom optical system according to the present invention which has the fourth or fifth composition is composed, in order from the object side, of a first lens unit which has a positive power or is powerless, a second lens unit which has a positive power, a third lens unit which has a positive power and a fourth lens unit which has a negative power, and characterized in that it is focused on an object located at a short distance by moving the second lens unit and the third lens unit toward the object side.

From a viewpoint of mechanisms such as that for moving lens units, it is ordinarily advantageous to focus a zoom optical system by moving a single lens unit.

Though the zoom optical system according to the present invention can be focused by moving only the third lens unit, it is difficult to obtain a zoom optical system which can meet the recent demand for expansion of a photographic range, and is composed of a small number of lens elements in particular and sufficiently satisfactory in its optical performance. It is difficult in particular to expand a photographic range for a zoom optical system which has a photographing magnification of ¼ at a tele position due to remarkable aggravation of spherical aberration.

When the zoom optical system according to the present invention is focused on an object located at an extremely short distance of 60 cm by moving the third lens unit toward the object side, spherical aberration and astigmatism may be aggravated. When the third lens unit on which a converging light bundle having passed through the second lens unit is incident on the third lens unit is moved for focusing, rays passing through the first negative lens element of the third lens unit are made higher, thereby producing positive spherical aberration in a large amount. This tendency is higher at the tele position.

When the second lens unit and the third lens unit are selected as focusing lens units, the zoom optical system according to the present invention can be focused by moving these lens units for short distances as described above. In this case, heights of rays passing through the lens elements are varied only a little by moving the lens units for focusing and the variations of aberrations can be reduced. Further, the short moving distances make it possible to configure compact the zoom optical system including a lens barrel.

In this case, it is preferable from a viewpoint of a lens barrel system to move the second lens unit and the third lens unit as an integral unit.

For the zoom optical system according to the present invention which has the fourth or fifth composition, it is desirable to dispose an aperture stop between the second lens unit and the third lens unit, and move the aperture stop for zooming independently of the lens units so as to widen an airspace between the aperture stop and the second lens unit. Speaking in short, the zoom optical system according to the present invention is composed, in order from the object side, of a first lens unit which has a positive power or is powerless, a second lens unit which has a positive power, a third lens unit which has a positive power and a fourth lens unit which has a negative power, and characterized in that an aperture is disposed between the second lens unit and the third lens unit, and moved independently toward the object side so as to widen an airspace between the aperture stop and the second lens unit for changing a magnification from a wide position to a tele position.

When an attempt is made to obtain a desired F number at a tele position of a zoom optical system which has a composition such as that of the optical system according to the present invention, an aperture stop has a large diameter. This is because the first lens unit of the zoom optical system according to the present invention has a relatively weak power and a light bundle which is nearly parallel is incident on the second lens unit. When the aperture stop has such a large diameter, a lens barrel has an enlarged diameter which is undesirable from viewpoints of a lens moving mechanism and a collapsing mechanism.

Further, it is demanded to reduce an F number at a tele position in particular for preventing image qualities from being degraded due to vibrations produced momentarily at photographing stages in association with shutter speeds when a focal length is long at the tele position and for configuring compact a strobe system including a capacitor, a power source, etc. by lowering strobe light intensity.

At the wide position of the zoom optical system according to the present invention, the aperture stop is disposed near the second lens unit for reducing a diameter of a front lens element while reserving a sufficient amount of offaxial rays (marginal rays) and at the tele position, the aperture stop is disposed at a location far from the second lens unit at which a light bundle converged by the second lens unit is thin so that a diameter of the aperture stop can be small at the tele position. A diameter of an axial incident light bundle is expressed as focal length/F number.

For changing a magnification of the zoom optical system according to the present invention, it is desirable to move the first lens unit and the fourth lens unit toward the object side, and then move the second lens unit and the third unit and with a time delay so as to widen an airspace between the second lens unit and the third lens unit. That is, variations of spherical aberration, curvature of field, chromatic aberration, etc. can be reduced by varying the airspace between the second lens unit and the third lens unit in the optical system which is composed of a small number of lens elements.

Though a portion of the second lens unit may be disposed on the image side of the aperture stop in the zoom optical system according to the present invention, it is preferable for simplifying a barrel which holds the lens elements and a stop mechanism to dispose the aperture stop on the image side of the second lens unit.

Variations of distortion or astigmatism can be reduced in the zoom optical system according to the present invention by configuring the second lens unit so as to have a surface which is located on the side of the aperture stop and concave toward the aperture stop. This reduction of the variation is more effective when the configuration of the second lens unit is combined with the disposition of the aperture stop on the image side of the second lens unit.

For the zoom optical system according to the present invention, it is desirable to configure a lens element which is adjacent to the aperture stop:on the image side so as to have a surface concave toward the aperture stop. This lens element makes it possible to adequately correct distortion and astigmatism. When the surface disposed on the image side of the aperture stop is an object side surface of the third lens unit in particular, the lens element produces an adequate influence on correction of aberrations by varying the airspace between the second lens unit and the third lens unit, thereby producing an advantage from viewpoints of manufacturing precision and a driving mechanism. It is more effective for correction of aberrations to dispose the second lens unit on the object side of the aperture stop, configure its surface on the side of the aperture stop as a concave surface, dispose the third lens unit on the image side of the aperture stop and configure its surface on the side of the aperture stop as a concave surface. That is, distortion and astigmatism can be corrected favorably by configuring surfaces on the object side and image side of the aperture stop as surfaces which are concave toward the aperture stop.

Further, it is desirable to use at least one aspherical surface in the lens component of the fourth lens unit in each composition of the zoom optical system according to the present invention.

For shortening a total length of a zoom optical system which is composed of four lens units such as that according to the present invention, it is effective to strengthen a power of a fourth lens unit. When the fourth lens unit is composed of a single lens component, lens elements have strong curvature, and it is desirable to correct aberrations of marginal rays such as curvature of field and distortion with aspherical surfaces.

When aspherical surfaces are used in the fourth lens unit for the purpose described above, it is desirable to use at least one aspherical surface which has such a shape as to moderate curvature toward a marginal portion.

Further, it is desirable to configure a negative lens component of the fourth lens unit so as to have a shape which satisfies the above-mentioned condition (2).

Furthermore, it is desirable that the fourth lens unit has a focal length f₄ which satisfies the above-mentioned condition (6).

In each composition of the zoom optical system according to the present invention, it is desirable to compose the first lens unit of a negative lens element and a positive lens element. This is a minimum requisite for correcting chromatic aberration produced by the fourth lens unit and imparting a required power for the zoom optical system. It is desirable to compose the first lens unit, in order from the object side, of a negative lens element which has a concave surface on the object side and a positive lens element which has a convex surface on the object side. When the first lens unit is composed as described above, it is possible to correct offaxial aberrations including chromatic aberration more effectively in consideration of the composition of the fourth lens unit.

Moreover, the first lens unit of the zoom optical system according to the present invention satisfies the following condition (11):

|f _(T) /f ₁|≦0.6  (11)

wherein the reference symbol f_(T) represents a focal length of the zoom optical system as a whole at its tele position and the reference symbol f₁ designates a focal length of the first lens unit.

If the upper limit of 0.6 of the condition (11) is exceeded, the first lens unit will have too strong a power, whereby aberrations of marginal rays will be aggravated remarkably in the vicinities of the tele position. Further, such too strong a power of the first lens unit will remarkably aggravate spherical aberration in the vicinities of the tele position in particular when the zoom optical system is focused on an object located at an extremely short distance by moving the second lens unit and the third lens unit as an integral unit, thereby making it difficult to shorten the extremely short distance.

It is more effective to configure the first lens unit so as to satisfy, in place of the above-mentioned condition (11), the following condition (11-1):

|f _(T) /f ₁|≦0.4  (11-1)

It is more preferable that the first lens unit has a positive power in the zoom optical system according to the present invention. In other words, it is desirable that the first lens unit satisfies the condition (11-1). If the first lens unit has a negative power, a front lens element will have a large diameter, whereby a camera will undesirably be large. Further, it is more desirable to adopt the upper limit of 0.4 as defined by the condition (11-1) in place of the upper limit of 0.6.

For the zoom optical system according to the present invention, it is desirable to compose the third lens unit, in order from the object side, of a positive lens element which has a concave surface on the object side and a positive lens element, and configure the positive lens elements as aspherical lens elements. The aspherical surfaces effectively correct variations of offaxial aberrations which are caused mainly by the fourth lens unit when a magnification is changed from the wide position to the tele position and provide an advantage for adequate correction of aberrations by adjusting the airspace between the second lens unit and the third lens unit which is made possible by configuring the object side surface of the third lens unit as the concave surface.

Further, selection of a plastic material for the positive lens elements makes it easy to lower a manufacturing cost of the third lens unit, lessen a weight of the third lens unit configure the lens elements as aspherical lens elements. By lessening the weight of the third lens unit, it is possible to lessen a burden on a moving mechanism drive system for focusing.

For minimizing production of chromatic aberration and offaxial aberrations in the third lens unit, it is desirable to compose this lens unit of a combination of a negative lens element and a positive lens element.

Further, it is desirable to select a plastic material for the negative lens element of the fourth lens unit for making it easy to lower a manufacturing cost, lessen a weight and configure the lens element as an aspherical lens element. Since the negative lens element of the fourth lens unit has the deep concave surface on the object side and a large diameter, it can be manufactured remarkably hardly when it is configured as an aspherical lens element. When a plastic material is selected for this lens element, it can be manufactured as an aspherical lens element relatively easily.

When a plastic material is selected for lens element to be disposed in the third lens unit and the fourth lens unit as described above, it is preferable to use the material for at least one positive lens element to be disposed in the third lens unit and a negative lens element to be disposed in the fourth lens unit.

When a pair of positive lens element and negative lens element are made of a plastic material, influences on focusing due to variations of temperature or humidity are cancelled with each other, thereby making it possible to reduce degradation of optical performance due to environmental variations. Further, a plastic material is preferable for lowering a manufacturing cost and lessening a weight.

Further, it is desirable to compose the second lens unit of the zoom optical system according to the present invention of a single lens element.

It is necessary to satisfy the condition (10) for reducing a diameter of a front lens element as described above. It is therefore preferable to configure the second lens unit so as to have a structural length as short as possible. The composition of the second lens unit of a single lens element is advantageous for composing the zoom optical system of a small number of lens elements and lessening a burden on a mechanism driving system for focusing (lessening a weight of the lens unit). Further, it is desirable to configure the lens element as a positive lens element which has a convex surface on the object side.

For the reason described above, it is desirable to compose the second lens unit of a single positive lens element which has a convex surface on the object side.

Furthermore, it is desirable that the zoom optical system according to the present invention satisfies the above-mentioned condition (4).

For configuring compact the zoom optical system according to the present invention, it is desirable to compose the optical system as a whole of six lens elements. Speaking more concretely, it is most desirable to compose the zoom optical system of a first lens unit which is composed of two lens elements, a second lens unit which is composed of a single lens element, a third lens unit which is composed of two lens elements and a fourth lens unit which is composed of a single lens element so that the optical system is compact, has high optical performance and can be manufactured at a low cost.

Moreover, it is preferable to configure the fourth lens unit not in a circular shape but in an oval shape reserving an effective portion. The zoom optical system can be compact by configuring the fourth lens unit in the oval shape.

An effective portion of a final lens element of the zoom optical system through which a required light bundle passes has a nearly rectangular shape which is similar to a shape of a film, or upper and lower portions of the final lens element don't serve for imaging a light bundle onto a film surface. Accordingly, a space for disposing a lens driving system, etc. can be formed by cutting off a portion 2 as shown in FIGS. 3A and 3B. Further, right and left side portions can also be cut off as shown in FIG. 3B. In FIGS. 3A and 3B, a reference numeral 1 represents an effective portion and a reference symbol L designates a lens element.

It is preferable to configure the negative lens component of the fourth lens unit as a cemented lens component which consists of a meniscus molded glass lens element having an aspherical surface and a spherical lens element. A refractive index and a shape of a plastic lens element are largely varied by temperature and humidity changes, and a refractive index and a shape of an aspherical surface are varied by temperature and humidity changes even when it is formed with a resin material on a glass base.

The zoom optical system according to the present invention which has an another composition is composed, in order from the object side: of a front lens group which is composed of a lens unit or a plurality of lens units moved along an optical axis for focusing or a magnification change and lens components, and has a positive power as a whole; and a rear lens group which has a negative power: at least one negative lens component disposed in the rear lens group being composed of a cemented lens component consisting of a meniscus molded glass lens element having an aspherical surface and a spherical lens element.

A refractive index and a shape of a plastic lens element are largely varied by temperature and humidity changes, and a refractive index and a shape of an aspherical surface are varied by temperature and humidity changes even when it is formed with a resin material on a glass base as described above. Large differences in physical properties such as hardness between a glass material and a plastic material make it difficult to work into an oval shape.

A glass material can be formed into a meniscus shape relatively easily and at a low cost, and a cemented lens component is not varied by temperature or humidity and can easily be worked.

For this reason, the zoom optical system according to the present invention which has this composition uses the cemented lens component consisting of the meniscus molded glass element having the aspherical surface and the spherical lens element in the rear lens group.

Further, it is desirable to configure the cemented lens component having the aspherical surface as an oval lens component which reserves a required effective portion.

The effective portion (a range through which a required light bundle passes) of the rear lens group has a shape which is similar to that of a film, and upper and lower portions of the rear lens group do not serve for imaging a light bundle onto a film surface. It is possible to dispose parts such as a lens driving system in a space formed by cutting off the portions which do not serve for imaging the light bundle. Needless to say, right and left side portions can also be cut off.

For the zoom optical system according to the present invention which has this composition, it is desirable to configure the front lens group so as to comprise at least one aspherical lens element which has an aspherical surface and form all aspherical lens elements by molding a glass material. When the front lens group is configured as described above, the zoom optical system according to the present invention is a compact optical system having optical performance which can hardly be affected by temperature and-humidity variations.

It is desirable that the zoom optical system according to the present invention satisfies, in it collapsed condition, the following condition (12):

0<D ₀(i)/D _(min)(i)<2  (12)

wherein the reference numeral D₀(i) (i=1, 2, 3 or 4) represents an airspace reserved between the lens units in the collapsed condition; D₀(1) being an airspace reserved between the first lens unit and the second lens unit, D₀(2) being an airspace reserved between the second lens unit and the third lens unit, D₀(3) being an airspace reserved between the third lens unit and the fourth lens unit and D₀(4) being an airspace reserved between the fourth lens unit and the image surface; and the reference symbol D_(min)(i) designates a minimum value of each airspace which is variable in the entire zooming region; D_(min)(1) being a minimum value of the airspace reserved between the first lens unit and the second lens unit, D_(min)(2) being a minimum value of the airspace reserved between the second lens unit and the third lens unit, D_(min)(3) being a minimum value of the airspace reserved between the third lens unit and the fourth lens unit and D_(min)(4) being a minimum value of the airspace reserved between the fourth lens unit and the image surface.

Now, the preferred embodiments of the zoom optical system according to the present invention will be described below in a form of numerical data:

Embodiment 1 f = 30.5˜50.0˜87.0, F number = 4.26˜6.97˜12.1 2ω = 57.6°˜37.6°˜22.2° r₁ = −33.415 d₁ = 2.000 n₁ = 1.84666 ν₁ = 23.78 r₂ = 147.224 d₂ = 0.100 r₃ = 25.297 d₃ = 3.469 n₂ = 1.55963 ν₂ = 61.17 r₄ = −68.702 d₄ = D₁ (variable) r₅ = 17.240 d₅ = 2.693 n₃ = 1.84666 ν₃ = 23.78 r₆ = 35.617 d₆ = 3.190 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −12.397 d₈ = 2.166 n₄ = 1.84666 ν₄ = 23.78 r₉ = −22.647 d₉ = 0.905 r₁₀ = 44.141 d₁₀ = 3.249 n₅ = 1.52542 ν₅ = 55.78 r₁₁ = −13.534 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −12.025 (aspherical surface) d₁₂ = 1.500 n₆ = 1.52542 ν₆ = 55.78 r₁₃ = 73.816 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = 0, E = 1.29274 × 10⁻⁴, F = 1.10773 × 10⁻⁷ G = 8.78090 × 10⁻⁹, H = 1.04715 × 10⁻¹⁰ (12th surface) K = −0.61890, E = 7.01015 × 10⁻⁵, F = −2.35355 × 10⁻⁷, G = 4.25966 × 10⁻⁹ H = −4.07875 × 10⁻¹¹ variation of airspaces for magnification change f 30.5 50.0 87.0 D₁ 0.255 3.818 5.665 D₂ 2.533 5.007 7.971 D₃ 11.849 5.812 1.000 D₄ 7.003 22.483 49.976

ΣD₄/y=0.09, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.72, ν_(R)=55.8 β_(4T)/β_(4W)=2.57, f_(BW)/f_(W)=0.23, f₄/f_(W)=0.64, β_(3T)32 0.69 y/f₁=0.002, |f4|/y=1.13, E(W)/f_(W)=0.28, |f_(T)/f₁|=0.009 D₀(1)/D_(min)(1)=1.00, D₀(2)/D_(min)(2)=1.00, D₀(3)/D_(min)(3)=1.00, D₀(4)/D_(min)(4)=1.00

Embodiment 2 f = 30.5˜50.0˜87.0, F number = 4.50˜6.93˜11.13 2ω = 57.6°˜38.6°˜22.8° r₁ = −24.110 d₁ = 2.000 n₁ = 1.84666 ν₁ = 23.78 r₂ = −47.573 d₂ = 0.100 r₃ = 24.424 d₃ = 2.680 n₂ = 1.58913 ν₂ = 61.14 r₄ = −1958.075 d₄ = D₁ (variable) r₅ = 39.944 d₅ = 2.298 n₃ = 1.84666 ν₃ = 23.78 r₆ = −46.110 d₆ = 0.200 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −15.350 d₈ = 1.500 n₄ = 1.84666 ν₄ = 23.78 r₉ = 663.553 d₉ = 2.190 r₁₀ = 41.169 d₁₀ = 4.256 n₅ = 1.51633 ν₅ = 64.14 r₁₁ = −11.673 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −12.077 (aspherical surface) d₁₂ = 1.500 n₆ = 1.51633 ν₆ = 64.14 r₁₃ = 55.236 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = 0, E = 1.19488 × 10⁻⁴, F = 2.93708 × 10⁻⁷ G = 3.56719 × 10⁻⁹, H = −2.39160 × 10⁻¹¹ (12th surface) K = −0.56706, E = 9.22160 × 10⁻⁵, F = 5.89930 × 10⁻⁷, G = −1.60795 × 10⁻⁸ H = 6.92449 × 10⁻¹¹ variation of airspaces for magnification change f 30.5 50.0 87.0 D₁ 4.567 11.092 18.709 D₂ 1.923 2.929 4.238 D₃ 12.092 6.087 1.000 D₄ 6.998 21.281 45.864

ΣD₄/y=0.09, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.64, ν_(R)=64.1 β_(4T)/β_(4W)=2.45, f_(BW)/f_(W)=0.23, f₄/f_(W)=0.62, β_(3T)=1.06 y/f₁=0.151, |f4|/y=1.10, E(W)/f_(W)=0.29, |f_(T)/f₁|=0.761 D₀(1)/D_(min)(1)=0.11, D₀(2)/D_(min)(2)=0.52, D₀(3)/D_(min)(3)=1.00, D₀(4)/D_(min)(4)=0.57

Embodiment 3 f = 30.5˜50.0˜87.0, F number = 4.69˜7.06˜10.36 2ω = 59.6°˜38.2°˜22.8° r₁ = −32.463 d₁ = 2.000 n₁ = 1.76182 ν₁ = 26.52 r₂ = −59.590 d₂ = 0.100 r₃ = 18.025 d₃ = 3.096 n₂ = 1.60311 ν₂ = 60.64 r₄ = 56.280 d₄ = D₁ (variable) r₅ = −22.857 (aspherical surface) d₅ = 4.075 n₃ = 1.52542 ν₃ = 55.78 r₆ = −16.117 d₆ = 0.200 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = 60.548 d₈ = 2.803 n₄ = 1.84666 ν₄ = 23.78 r₉ = 36.519 d₉ = 1.201 r₁₀ = −1796.395 d₁₀ = 2.790 n₅ = 1.51633 ν₅ = 64.14 r₁₁ = −14.086 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −12.913 (aspherical surface) d₁₂ = 1.500 n₆ = 1.48749 ν₆ = 70.23 r₁₃ = 46.171 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (5th surface) K = 0, E = −1.18339 × 10⁻⁴, F = −9.04268 × 10⁻⁷ G = 3.98631 × 10⁻⁸, H = 0 (11th surface) K = 0, E = 5.31821 × 10⁻⁵, F = −3.78901 × 10⁻⁷, G = 1.47543 × 10⁻⁸, H = 0 (12th surface) K = −0.54800, E = 1.11357 × 10⁻⁴, F = 5.01932 × 10⁻⁷, G = −1.00759 × 10⁻⁸, H = 4.60521 × 10⁻¹¹ variation of airspaces for magnification change f 30.5 50.0 87.0 D₁ 1.779 7.191 16.524 D₂ 3.459 1.892 5.052 D₃ 11.602 6.098 1.053 D₄ 6.999 23.224 44.070

ΣD₄/Y=0.09, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.56, ν_(R)=70.2 β_(4T)/β_(4W)=2.30, f_(BW)/f_(W)=0.23, f₄/f_(W)=0.67, β_(3T)=0.58 y/f₁=0.234, |f4|/y=1.19, E(W)/f_(W)=0.26, |f_(T)f₁|=1.177

Embodiment 4 f = 30.5˜60.0˜117.0, F number = 3.90˜7.04˜11.71 2ω = 59.6°˜31.6°˜16.8° r₁ = 30.833 d₁ = 4.166 n₁ = 1.84666 ν₁ = 23.78 r₂ = 24.289 d₂ = 0.100 r₃ = 22.307 d₃ = 3.580 n₂ = 1.48749 ν₂ = 70.23 r₄ = 56.120 d₄ = D₁ (variable) r₅ = ∞ (stop) d₅ = 1.691 r₆ = −10.374 d₆ = 1.500 n₃ = 1.63930 ν₃ = 44.87 r₇ = −18.850 d₇ = 0.200 r₈ = 49.204 d₈ = 3.256 n₄ = 1.56384 ν₄ = 60.67 r₉ = −11.983 (aspherical surface) d₉ = D₂ (variable) r₁₀ = −165.021 d₁₀ = 1.500 n₅ = 1.78800 ν₅ = 47.37 r₁₁ = 25.722 d₁₁ = 1.769 r₁₂ = −379.466 d₁₂ = 4.269 n₆ = 1.60311 ν₆ = 60.64 r₁₃ = −12.261 d₁₃ = D₃ (variable) r₁₄ = −11.302 (aspherical surface) d₁₄ = 1.500 n₇ = 1.48749 ν₇ = 70.23 r₁₅ = 55.984 d₁₅ = D₄ (variable) r₁₆ = ∞ (image) aspherical surface coefficients (9th surface) K = 1.34221, E = 2.75220 × 10⁻⁴, F = 6.11657 × 10⁻⁷, G = 6.53307 × 10⁻⁸, H = −6.04534 × 10⁻¹⁰ (14th surface) K = −0.09533, E = 1.04960 × 10⁻⁴, F = 1.20141 × 10⁻⁷, G = 5.65953 × 10⁻⁹, H = 0 variation of airspaces for magnification change f 30.5 60.0 117.0 D₁ 1.147 10.942 26.870 D₂ 3.321 1.706 0.200 D₃ 10.057 4.613 2.047 D₄ 6.998 30.414 67.350

ΣD₄/Y=0.09, (r_(F)+r_(R))/(r_(F)−r_(R))=−0. 66, ν_(R)=70.2 β_(4T)/β4W=3.23, f_(BW)/f_(W)0.23, f₄/f_(W) =0.63, β_(3T)=0.82 y/f₁=0.129, |f4|/y=1.11, E(W)/f_(W)=0.22, |f_(T)/f₁|=0.870

Embodiment 5 f = 30.5˜60.0˜117.0, F number = 3.27˜6.43˜12.52 2ω = 61.6°˜33.2°˜16.8° r₁ = 17.684 d₁ = 2.000 n₁ = 1.80518 ν₁ = 25.42 r₂ = −48.592 d₂ = 0.100 r₃ = 115.032 d₃ = 3.313 n₂ = 1.51633 ν₂ = 64.14 r₄ = −24.247 d₄ = D₁ (variable) r₅ = ∞ (stop) d₅ = 0.800 r₆ = 181.092 d₆ = 5.000 n₃ = 1.84666 ν₃ = 23.78 r₇ = −50.066 d₇ = D₂ (variable) r₈ = −17.228 (aspherical surface) d₈ = 5.000 n₄ = 1.51633 ν₄ = 64.14 r₉ = −12.792 d₉ = 0.200 r₁₀ = −44.027 d₁₀ = 3.280 n₅ = 1.80518 ν₅ = 25.42 r₁₁ = 56.132 d₁₁ = 4.782 n₆ = 1.56883 ν₆ = 56.36 r₁₂ = −15.554 d₁₂ = D₃ (variable) r₁₃ = −20.097 (aspherical surface) d₁₃ = 1.5000 n₇ = 1.72916 ν₇ = 54.68 r₁₄ = 51.095 d₁₄ = D₄ (variable) r₁₅ = ∞ (image) aspherical surface coefficients (8th surface) K = 0.32946, E = −1.55754 × 10⁻⁴, F = −1.24055 × 10⁻⁶, G = 2.57622 × 10⁻⁸, H = −4.82018 × 10⁻¹⁰ (13th surface) K = −0.28327, E = 4.34900 × 10⁻⁵, F = −3.75099 × 10⁻⁸, G = 3.31480 × 10⁻¹⁰, H = −3.16708 × 10⁻¹² variation of airspaces for magnification change f 30.5 60.0 117.0 D₁ 1.000 10.563 19.517 D₂ 5.617 14.145 18.217 D₃ 13.984 5.520 0.200 D₄ 6.996 25.834 62.591

ΣD₄/y=0.09, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.44, ν_(R)=54.7 β_(4T)/β_(4W)=3.04, f_(BW)/f_(W)=0.23, f₄/f_(W)=0.64, ν_(3T)=0.66 y/f₁=0.002, |f4|/y=1.13, E(W)/f_(W)=0.13, |f_(T)/f₁|=0.014

Embodiment 6 f = 30.5˜50.0˜87.0, F number = 4.48˜6.43˜10.06 2ω = 57.6°˜37.0°˜22.2° r₁ = 15.733 d₁ = 4.007 n₁ = 1.48960 ν₁ = 68.53 r₂ = 42.487 d₂ = 1.500 n₂ = 1.84666 ν₂ = 23.78 r₃ = 32.035 d₃ = D₁ (variable) r₄ = 38.650 d₄ = 2.345 n₃ = 1.84666 ν₃ = 23.78 r₅ = 97.253 d₅ = D₂ (variable) r₆ = −16.046 d₆ = 2.729 n₄ = 1.84666 ν₄ = 23.78 r₇ = −54.905 d₇ = 0.200 r₈ = ∞ (stop) d₈ = 3.153 r₉ = 60.542 d₉ = 3.449 n₅ = 1.75581 ν₅ = 44.04 r₁₀ = −17.190 (aspherical surface) d₁₀ = D₃ (variable) r₁₁ = −20.641 (aspherical surface) d₁₁ = 0.300 n₆ = 1.52288 ν₆ = 52.50 r₁₂ = −25.593 d₁₂ = 1.500 n₇ = 1.72916 ν₇ = 54.68 r₁₃ = 70.216 d₁₃ = D₄ (variable) r₄ = ∞ (image) aspherical surface coefficients (10th surface) K = 0, E = 7.87194 × 10⁻⁵, F = −8.24497 × 10⁻⁷, G = 3.55424 × 10⁻⁸, H = −4.63116 × 10⁻¹⁰ (11th surface) K = 0.79521, E = 8.41455 × 10⁻⁵, F = −1.43845 × 10⁻⁷, G = 4.10744 × 10⁻⁹, H = −2.90057 × 10⁻¹¹ variation of airspaces for magnification change f 30.5 50.0 87.0 D₁ 1.132 8.191 14.285 D₂ 2.268 1.728 0.610 D₃ 12.496 5.976 1.000 D₄ 5.997 20.397 47.182

ΣD₄/y=0.10, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.47, ν_(R)=54.7 β_(4T)/β_(4W)=2.40, f_(BF)/f_(W)0.20, f₄/f_(W)=0.74, β_(3T)=0.68 y/f₁=0.267, |f4|/y=1.31, E(W)/f_(W)=0.45, |f_(T)/f₁|=1.343

Embodiment 7 f = 30.5˜50.0˜87.0, F number = 4.62˜7.49˜11.79 2ω = 58.0°˜38.2°˜22.6° r₁ = 14.265 (aspherical surface) d₁ = 2.877 n₁ = 1.48749 ν₁ = 70.23 r₂ = 16.408 d₂ = D₁ (variable) r₃ = −40.180 (aspherical surface) d₃ = 5.000 n₂ = 1.84666 ν₂ = 23.78 r₄ = −33.347 d₄ = D₂ (variable) r₅ = ∞ (stop) d₅ = 1.363 r₆ = −12.206 d₆ = 1.500 n₃ = 1.84666 ν₃ = 23.78 r₇ = −24.830 d₇ = 0.200 r₈ = 111.808 d₈ = 4.395 n₄ = 1.74320 ν₄ = 49.34 r₉ = −13.524 (aspherical surface) d₉ = D₃ (variable) r₁₀ = −28.673 (aspherical surface) d₁₀ = 0.300 n₅ = 1.52288 ν₅ = 52.50 r₁₁ = −28.814 d₁₁ = 1.500 n₆ = 1.48749 ν₆ = 70.23 r₁₂ = 34.894 d₁₂ = D₄ (variable) r₁₃ = ∞ (image) aspherical surface coefficients (1th surface) K = −0.04241, E = −1.95169 × 10⁻⁶, F = −5.29827 × 10⁻⁸, G = 1.31657 × 10⁻⁹, H = −1.16614 × 10⁻¹¹ (3th surface) K = 0, E = −3.73845 × 10⁻⁵, F = 4.21185 × 10⁻⁷, G = −9.35462 × 10⁻⁹, H = 8.25452 × 10⁻¹¹ (9th surface) K = 0, E = 5.79527 × 10⁻⁵, F = −2.68017 × 10⁻⁷, G = 4.14949 × 10⁻⁸, H = −2.00555 × 10⁻⁹ (10th surface) K = 2.28144, E = 5.91867 × 10⁻⁵, F = −9.37737 × 10⁻⁷, G = 1.10034 × 10⁻⁸, H = −5.17760 × 10⁻¹¹ variation of airspaces for magnification change f 30.5 50.0 87.0 D₁ 2.636 9.810 21.425 D₂ 4.290 0.484 0.800 D₃ 17.148 7.321 1.000 D₄ 6.891 31.533 69.988

ΣD₄/y=0.10, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.10, ν_(R)=70.2 β_(4T)/β_(4W)=2.59, f_(BW)/f_(W)=0.23, f₄/f_(W)=1.05, β_(3T)=0.29 Y/f₁=0.111, |f4|/y=1.85, E(W)/f_(W)=0.43, |f_(T)/f₁|=0.559

Embodiment 8 f = 39.1 ˜ 75.0 ˜ 145.5, F number = 4.36 ˜ 6.70 ˜ 11.00 2ω = 46.4° ˜ 26.0° ˜ 13.6° r₁ = −28.390 d₁ = 2.494 n₁ = 1.84666 ν₁ = 23.78 r₂ = −92.579 d₂ = 0.125 r₃ = 85.188 d₃ = 3.571 n₂ = 1.48749 ν₂ = 70.23 r₄ = −33.911 d₄ = D₁ (variable) r₅ = 26.716 d₅ = 2.660 n₃ = 1.84666 ν₃ = 23.78 r₆ = 52.926 d₆ = 5.303 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −16.233 d₈ = 1.500 n₄ = 1.84666 ν₄ = 23.78 r₉ = −28.266 d₉ = 1.211 r₁₀ = 61.727 d₁₀ = 5.000 n₅ = 1.52542 ν₅ = 55.78 r₁₁ = −16.849 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −14.163 (aspherical surface) d₁₂ = 2.000 n₆ = 1.52542 ν₆ = 55.78 r₁₃ = 81.186 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = 0, E = 3.49942 × 10⁻⁵, F = 4.49980 × 10⁻⁷, G = 3.33849 × 10⁻¹⁰, H = −1.91736 × 10⁻¹⁰ (12th surface) K = −0.64236, E = 2.55484 × 10⁻⁵, F = 7.33897 × 10⁻⁷, G = −1.36011 × 10⁻⁸, H = 5.71927 × 10⁻¹¹ variation of airspaces for magnification change f 39.1 75.0 145.5 D₁ 0.200 9.132 17.978 D₂ 3.297 13.431 20.926 D₃ 18.629 8.495 1.000 D₄ 7.000 27.419 64.287

σD₄/y=0.12, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.70, ν_(R)55.78 β_(4T)/β_(4W)=2.85, f_(BW)/f_(W)=0.18, f₄/f_(W)=0.58, β_(3T)=0.70 y/f₁=0.020, |f4|/y=1.32, E(W)/f_(W)=0.27, |f_(T)/f₁|=0.167

Embodiment 9 f = 25.8 ˜ 50.0 ˜ 97.0, F number = 4.6 ˜ 6.6 ˜ 9.5 2ω = 66.50° ˜ 39.26° ˜ 20.46° r₁ = −27.1166 d₁ = 1.5000 n₁ = 1.84666 ν₁ = 23.78 r₂ = −77.9057 d₂ = 0.2762 r₃ = 102.5940 d₃ = 2.6646 n₂ = 1.48749 ν₂ = 70.23 r₄ = −32.0143 d₄ = D₁ (variable) r₅ = 13.2780 d₅ = 1.9957 n₃ = 1.72825 ν₃ = 28.46 r₆ = 20.3381 d₆ = 4.4624 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −10.2463 d₈ = 1.2235 n₄ = 1.80518 ν₄ = 25.42 r₉ = −15.4261 d₉ = 1.2066 r₁₀ = 27.0204 d₁₀ = 4.2278 n₅ = 1.51633 ν₅ = 64.14 r₁₁ = −12.1006 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −10.2640 (aspherical surface) d₁₂ = 1.5000 n₆ = 1.69680 ν₆ = 55.53 r₁₃ = 483.1490 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = 0.1841, E = 1.6352 × 10 ⁻⁴, F = 6.2157 × 10⁻⁷, G = −1.7728 × 10⁻¹⁰, H = −8.1699 × 10⁻¹¹ (12th surface) K = −1.3391, E = 2.1631 × 10 ⁻⁵, F = −1.5789 × 10 ⁻¹⁰, G = −7.9115 × 10 ⁻⁹, H = 4.2279 × 10⁻¹² variation of airspaces for magnification change f 25.8 50.0 97.0 D₁ 0.49468 7.33918 14.45283 D₂ 1.39532 6.13105 10.62890 D₃ 10.93606 5.56265 1.95054 D₄ 4.99560 20.29303 46.91614

y=17.30, f₁=1074.15, ΣD₄=1.50, f₄=−14.41 β_(4T)=4.32, β_(4W)=1.41, f_(BW)=5.00, f_(W)=25.80 y/f₁=0.016, ΣD₄/y=0.087, |f₄|/y=0.833, ν_(R)=55.530 β_(4T)/β_(4W)=3.069, f_(BW)/f_(W)=0.194, |β_(3T)|=0.522 (r_(F)+r_(R))/(r_(F)−r_(R))=−0.96, f₄/f_(W)=0.56, E(W)/f_(W)=0.36 |f_(T)/f₁|=0.090

Embodiment 10 f = 25.8 ˜ 50.0 ˜ 97.0, F number = 4.6 ˜ 6.6 ˜ 9.5 2 ω = 66.82° ˜ 39.00° ˜ 20.54° r₁ = −26.9886 d₁ = 1.5000 n₁ = 1.84666 ν₁ = 23.78 r₂ = −79.3757 d₂ = 0.2764 r₃ = 95.4591 d₃ = 2.5060 n₂ = 1.48749 ν₂ = 70.23 r₄ = −33.7409 d₄ = D₁ (variable) r₅ = 13.1491 d₅ = 1.9920 n₃ = 1.71736 ν₃ = 29.51 r₆ = 20.7672 d₆ = 4.8070 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −10.6979 d₈ = 1.2731 n₄ = 1.80518 ν₄ = 25.42 r₉ = −17.4594 d₉ = 0.3457 r₁₀ = 32.4289 d₁₀ = 1.9994 n₅ = 1.53172 ν₅ = 48.84 r₁₁ = −59.7777 d₁₁ = 0.7706 r₁₂ = 121.1517 d₁₂ = 3.0524 n₆ = 1.51633 ν₆ = 64.14 r₁₃ = −13.2184 (aspherical surface) d₁₁ = D₃ (variable) r₁₄ = −9.7829 (aspherical surface) d₁₄ = 1.5000 n₇ = 1.69680 ν₇ = 55.53 r₁₅ = 282.8806 d₁₅ = D₄ (variable) r₁₆ = ∞ (image) aspherical surface coefficients (13th surface) K = −0.1264, E = 1.3930 × 10⁻⁴, F = 8.8210 × 10⁻⁸, G = 4.3852 × 10⁻⁹, H = 2.0624 × 10⁻¹⁰ (14th surface) K = −1.2746, E = 3.1937 × 10 ⁵, F = 3.9147 × 10⁻⁷, G = −1.7833 × 10⁻⁸, H = 6.3622 × 10⁻¹¹ variation of airspaces for magnification change f 25.8 50.0 97.0 D₁ 0.50481 6.54922 13.59051 D₂ 1.47742 6.36732 10.52597 D₃ 9.66820 4.70712 1.41972 D₄ 5.24358 20.03919 46.37990

y=17.30, f₁ =9999.58, ΣD ₄=1.50, f₄=−13.54 β_(4T)=4.49, β_(4W)=1.45, f_(BW)=5.24, f_(W)=25.80 y/f₁=0.002, ΣD₄/y=0.087, |f₄|/y=0.783, ν_(R)55.530 β_(4T)/β_(4W)=3.095, f_(BW)/f_(W)=0.203, |β_(3T)|=0.508 (r_(F)+r_(R))/(r_(F)−r_(R))=−0.93, f₄/f_(W)=0.53, E(W)/f_(W)=0.38 |f_(T)/f₁|=0.010

Embodiment 11 f = 23.2 ˜ 45.0 ˜ 87.3, E number = 4.6 ˜ 7.3 ˜ 11.5 2ω = 74.86° ˜ 42.70° ˜ 23.08° r₁ = −26.6265 d₁ = 1.5000 n₁ = 1.84666 ν₁ = 23.78 r₂ = −60.3264 d₂ = 0.2589 r₃ = 67.8623 d₃ = 3.2800 n₂ = 1.48749 ν₂ = 70.23 r₄ = −37.1229 d₄ = D₁ (variable) r₅ = 12.4220 d₅ = 2.0932 n₃ = 1.72825 ν₃ = 28.46 r₆ = 16.6622 d₆ = 2.8917 r₇ = ∞ (Stop) d₇ = D₂ (variable) r₈ = 9.1930 d₈ = 1.4935 n₄ = 1.80518 ν₄ = 25.43 r₉ = −12.6836 d₉ = 0.2000 r₁₀ = 22.9266 d₁₀ = 5.4107 n₅ = 1.48749 ν₅ = 70.23 r₁₁ = −10.8680 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −9.8042 (aspherical surface) d₁₂ = 1.5000 n₆ = 1.72916 ν₆ = 54.68 r₁₃ = 1636.6644 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = 0, E = 1.9704 × 10⁻⁴, F = 1.7680 × 10⁻⁶, G = −2.4167 × 10 ⁻⁸, H = −1.8315 × 10⁻¹⁶ (12th surface) K = −1.6076, E = −4.4969 × 10 ⁻⁶, F = 1.1775 × 10 ³¹ ⁶, G = −2.4335 × 10⁻⁸, H = 8.7355 × 10⁻¹¹ variation of airspaces for magnification change f 23.2 45.0 87.3 D₁ 0.55421 6.77774 15.83360 D₂ 2.13876 7.28479 12.01005 D₃ 9.56067 4.75116 1.48506 D₄ 4.49962 17.76807 39.59696

y=17.30, f₁=261.74, ΣD₄=1.50, f₄=−13.36 β_(4T)=4.03, β_(4W)=1.40, f_(BW)=4.50, f_(W) =23.20 y/f ₁=0.066, ΣD₄/y=0.087, |/f₄|y=0.772, ν_(R)=54.680 β_(4T)/β_(4W)=2.875, f_(BW)/f_(W)=0.194, |β_(3T)|=0.475 (r_(F)+r_(R))/(r_(F)−r_(R))=−0.99, f₄/f_(W)=0.58, E(W)/f_(W)=0.35 |f_(T)/f₁|=0.334

Embodiment 12 f = 23.3 ˜ 47.7 ˜ 97.0, F number = 4.6 ˜ 7.3 ˜ 11.5 2ω = 73.60° ˜ 41.58° ˜ 20.64° r_(1 = −26.8442) d₁ = 1.5000 n₁ = 1.84666 ν₁ = 23.78 r₂ = −70.5797 d₂ = 0.1449 r₃ = 37.4414 d₃ = 3.1808 n₂ = 1.48749 ν₂ = 70.23 r₄ = −64.0264 d₄ = D₁ (variable) r₅ = 12.7493 (aspherical surface) d₅ = 2.0195 n₃ = 1.72825 ν₃ = 28.46 r₆ = 18.8406 d₆ = 3.0428 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −9.1301 d₈ = 1.5428 n₄ = 1.80518 ν₄ = 25.42 r₉ = −12.3479 d₉ = 0.2000 r₁₀ = 19.8198 d₁₀ = 5.2664 n₅ = 1.48749 ν₅ = 70.23 r₁₁ = −12.2303 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −9.6622 (aspherical surface) d₁₂ = 1.5000 n₆ = 1.72916 ν₆ = 54.68 r₁₃ = 1270.6906 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (5th surface) K = 0, E = 5.4751 × 10⁻⁶, F = 3.0824 × 10⁻⁷, G = −4.8250 × 10⁻⁹, H = −1.8072 × 10⁻¹³ (11th surface) K = −0.0649, E = 1.9397 × 10 ⁻⁴, F = 1.0963 × 10⁻⁶, G = −5.2102 × 10⁻⁸, H = 7.7101 × 10⁻¹⁰ (12th surface) K = −1.1814, E = 5.8573 × 10⁻⁵, F = 2.7718 × 10⁻⁷, G = −1.7293 × 10 ⁻⁸, H = 3.3709 × 10⁻¹¹ variation of airspaces for magnification change f 23.3 47.7 97.0 D₁ 0.54306 7.07095 12.94157 D₂ 2.14139 6.13960 9.46476 D₃ 9.12343 4.10938 1.09997 D₄ 4.50047 20.40028 50.07177

y=17.30, f₁=481.08, ΣD₄=1.50, f₄=−13.14 β_(4T)=4.87, β_(4W)=1.41, f_(BW)=4.50, f_(W)=23.30 y/f₁=0.036, ΣD₄/y=0.087, |f₄|/y=0.760, ν_(R)=54.680 β_(4T)/β_(4W)=3.463, f_(BW)/f_(W)=0.193, |β_(3T)|=0.468 (r_(F)+r_(R))/(r_(F)−r_(R))=−0.98, f₄/f_(W)=0.56, E(W)/f_(W)=0.35 |f_(T)/f₁|=0.202

Embodiment 13 f = 25.8 ˜ 55.9 ˜ 121.2, F number = 4.6 ˜ 6.7 ˜ 10.5 2ω = 66.38° ˜ 35.24° ˜ 16.64° r₁ = −27.6313 d₁ = 1.5000 n₁ = 1.84666 ν₁ = 23.78 r₂ = −70.3169 d₂ = 0.2942 r₃ = 150.1397 d₃ = 2.2750 n₂ = 1.48749 ν₂ = 70.23 r₄ = −34.1618 d₄ = D₁ (variable) r₅ = 13.6177 d₅ = 1.9779 n₃ = 1.72151 ν₃ = 29.24 r₆ = 20.9041 d₆ = 5.0142 r₇ = μ (stop) d₇ = D₂ (variable) r₈ = −9.9762 d₈ = 1.2942 n₄ = 1.80518 ν₄ = 25.42 r₉ = −15.6923 d₉ = 0.8147 r₁₀ = 25.5479 d₁₀ = 4.2347 n₅ = 1.51823 ν₅ = 58.96 r₁₁ = −11.3640 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −9.8169 (aspherical surface) d₁₂ = 1.5000 n₆ = 1.69680 ν₆ = 55.53 r₁₃ = 1168.0658 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = 0.1473, E = 1.8652 × 10⁻⁴, F = −7.8672 × 10 ⁻⁸, G = 1.1264 × 10⁻⁸, H = #8.3800 × 10⁻¹¹ (12th surface) K = −1.3386, E = 2.3993 × 10⁻⁵, F = −2.1307 × 10⁻⁷, G = −8.2513 × 10⁻⁹, H = 7.0584 × 10⁻¹² variation of airspaces for magnification change f 25.8 55.9 121.2 D₁ 0.49485 8.81731 17.24620 D₂ 1.46761 7.40303 12.00263 D₃ 11.26661 5.43138 1.90381 D₄ 4.83931 23.19350 59.95041

y=17.30, f₁=13767.40, ΣD₄=1.53, f₄=−13.96 β_(4T)=5.36, β_(4W)=1.41, f_(BW)=4.84, f_(W)=25.80 y/f₁=0.001, ΣD₄/y=0.088, |f ₄|/y=0.807, ν_(R)=55.530 β_(4T)/β_(4W)=3.800, f_(BW)/f_(W)=0.188, |β_(3T)|=0.491 (r_(F)+r_(R))/(r_(F)−r_(R))=−0.98, f₄/f_(W)=0.54, E(W)/f_(W)0.38 |f_(T)/f₁|=0.009

Embodiment 14 f = 25.8 ˜ 50.0 ˜ 97.0, F number = 4.6 ˜ 6.6 ˜ 9.5 2ω = 66.14° ˜ 38.62° ˜ 20.36° r₁ = −26.6127 d₁ = 1.4986 n₁ = 1.84666 ν₁ = 23.78 r₂ = −81.1028 d₂ = 0.0587 r₃ = 139.8794 d₃ = 3.3208 n₂ = 1.48749 ν₂ = 70.23 r₄ = −29.5110 d₄ = D₁ (variable) r₅ = 13.1607 d₅ = 1.9087 n₃ = 1.71736 ν₃ = 29.51 r₆ = 22.2256 d₆ = 4.8712 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −10.2430 d₈ = 2.2655 n₄ = 1.80518 ν₄ = 25.42 r₉ = −16.1242 d₉ = 0.2483 r₁₀ = 26.8390 d₁₀ = 3.7722 n₅ = 1.51633 ν₅ = 64.14 r₁₁ = −13.3135 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −10.9326 (aspherical surface) d₁₂ = 0.2775 n₆ = 1.52288 ν₆ = 52.51 r₁₃ = −12.6856 d₁₃ = 1.2500 n₇ = 1.75500 ν₇ = 52.32 r₁₄ = −1.454 × 10 ⁵ d₁₄ = D₄ (variable) r₁₅ = ∞ (image) aspherical surface coefficients (11th sur_(face)) K = −0.0539, E = 1.3858 × 10⁻⁴, F = −8.0346 × 10 ⁻⁷, G = 1.6995 × 10 ⁻⁸, H = −1.0963 × 10⁻¹⁰ (12th surface) K = −1.3032, E = 6.5513 × 10 ⁻⁵, F = −6.6160 × 10 ⁻⁷, G = 4.4871 × 10⁻¹⁰, H = −4.2205 × 10 ⁻¹¹ variation of airspaces for magnification change f 25.8 50.0 97.0 D₁ 0.94023 8.03156 13.85150 D₂ 2.21302 6.82114 10.36168 D₃ 11.25002 5.25611 1.37851 D₄ 4.65403 20.34403 48.97025

y=17.30, f₁=481.08, ΣD₄=1.50, f₄=−15.09 β_(4T)=4.30, β_(4W)=1.36, f_(BW)=4.65, f_(W)=25.80 y/f₁=0.036, ΣD₄/y=0.087, |f₄|/y=0.872, ν_(R)=52.320 β_(4T)/β_(4W)=3.153, f_(BW)/f_(W)=0.180, |β_(3T)|=0.583 (r_(F)+r_(R))/(r_(F)−r_(R))=−1.00, f₄/f_(W)=0.59, E(W)/f_(W)=0.40 |f_(T)/f₁|=0.008

Embodiment 15 f = 39.14˜67.50˜116.40, F number = 4.64˜7.08˜10.82 2ω = 56.4°˜35.0°˜21.0° r₁ = −43.8601 d₁ = 1.8000 n₁ = 1.78472 ν₁ = 25.68 r₂ = −1030.7853 d₂ = 0.1500 r₃ = 24.1803 d₃ = 2.5000 n₂ = 1.51823 ν₂ = 58.90 r₄ = 139.6404 d₄ = D₁ (variable) r₅ = 29.5852 d₅ = 2.3000 n₃ = 1.67270 ν₃ = 32.10 r₆ = 206.6298 d₆ = 0.7000 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −15.7528 d₈ = 1.6000 n₄ = 1.78472 ν₄ = 25.68 r₉ = −23.7259 d₉ = 3.4834 r₁₀ = 221.9716 d₁₀ = 4.0000 n₅ = 1.52542 ν₅ = 55.78 r₁₁ = −16.3581 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −15.0483 (aspherical surface) d₁₂ = 1.9000 n₆ = 1.52542 ν₆ = 55.78 r₁₃ = 96.7496 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = 0.5560, E = 7.1407 × 10⁻⁵, F = 4.1778 × 10⁻⁷, G = 3.9989 × 10⁻⁹, H = 4.8052 × 10⁻¹¹ (12th surface) K = −1.1777, E = 1.7761 × 10⁻⁵, F = 2.7425 × 10⁻⁷, G = −3.7741 × 10⁻⁹, H = 1.1455 × 10⁻¹¹ variation of airspaces for magnification change f 39.14 67.50 116.40 D₁ 0.600 3.430 8.885 D₂ 3.234 7.523 10.641 D₃ 16.160 8.118 2.800 D₄ 9.668 31.629 68.273

ΣD₄/y=0.09, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.73, ν_(R)=55.78, β_(4T)/β_(4W)=2.66, f_(BW)/f_(W)=0.25, f₄/f_(W)=0.59, β_(3T)=0.63 y/f₁=0.022, |f₄|/y=1.14, E(W)/f_(W)=0.14, |f_(T)/f₁=0.116

Embodiment 16 f = 39.14˜67.50˜116.40, F number = 4.64˜7.08˜10.82 2ω = 57.2°˜35.0°˜21.0° r₁ = −44.9276 d₁ = 1.8000 n₁ = 1.78472 ν₁ = 25.68 r₂ = 2003.3044 d₂ = 0.1500 r₃ = 22.6790 d₃ = 2.3000 n₂ = 1.51823 ν₂ = 58.90 r₄ = 117.8594 d₄ = D₁ (variable) r₅ = 26.2458 d₅ = 2.1000 n₃ = 1.67270 ν₃ = 32.10 r₆ = 140.9926 d₆ = 0.9000 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −16.0819 d₈ = 1.6000 n₄ = 1.78472 ν₄ = 25.68 r₉ = −24.1717 d₉ = 3.5273 r₁₀ = 151.7049 d₁₀ = 3.8000 n₅ = 1.52542 ν₅ = 55.78 r₁₁ = −17.7563 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −14.9780 (aspherical surface) d₁₂ = 1.9000 n₆ = 1.52542 ν₆ = 55.78 r₁₃ = 109.9367 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = 0.5472, E = 6.8034 × 10⁻⁵, F = 2.2151 × 10⁻⁷, G = 1.8928 × 10⁻⁹, H = 4.3557 × 10⁻¹¹ (12th surface) K = −1.1762, E = 1.6846 × 10⁻⁵, F = 4.7752 × 10⁻⁸, G = −5.6211 × 10⁻¹⁰, H = 4.6330 × 10⁻¹³ f 39.14 67.50 116.40 variation of airspaces for magnification change D₁ 2.000 4.347 8.685 D₂ 2.877 7.032 9.529 D₃ 15.646 7.324 2.000 D₄ 9.708 32.037 70.143 variation of airspaces for focusing D₁ 0.614 2.734 6.813 D₂ 2.877 7.032 9.529 D₃ 17.032 8.936 3.872 D₄ 9.708 32.037 70.143

ΣD₄/y=0.09, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.76, ν_(R)=55.78, β_(4T)/β_(4W)=2.69, f_(BW)/f_(W)=0.25, f₄/f_(W)=0.64, β_(3T)=0.67, y/f₁=0.022, |f₄|/y=1.16, E(W)/f_(W)=0.17, |f_(T)/f₁=0.116

Embodiment 17 f = 32.31˜62.52˜121.27, F number = 4.60˜6.95˜10.50 2ω = 66.0°˜37.4°˜20.0° r₁ = −39.7441 d₁ = 1.8754 n₁ = 1.84666 ν₁ = 23.78 r₂ = −210.6045 d₂ = 0.2946 r₃ = 115.2842 d₃ = 2.9875 n₂ = 1.48749 ν₂ = 70.23 r₄ = −37.5782 d₄ = D₁ (variable) r₅ = 15.6256 d₅ = 2.0509 n₃ = 1.72825 ν₃ = 28.46 r₆ = 26.2181 d₆ = 2.5467 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −13.9564 d₈ = 1.8289 n₄ = 1.80518 ν₄ = 25.42 r₉ = −22.6087 d₉ = 2.1450 r₁₀ = 59.3377 d₁₀ = 3.8820 n₅ = 1.51633 ν₅ = 64.14 r₁₁ = −14.5766 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −13.4744 (aspherical surface) d₁₂ = 1.8754 n₆ = 1.69680 ν₆ = 55.53 r₁₃ = −504.2855 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = −1.1382, E = 2.5110 × 10⁻⁵, F = 3.1102 × 10⁻⁷, G = 1.2324 × 10⁻⁹, H = −6.0277 × 10⁻¹¹, I = 2.0990 × 10⁻¹³ (12th surface) K = −0.7202, E = 1.8054 × 10⁻⁵, F = 2.0045 × 10⁻⁷, G = −1.6830 × 10⁻⁹, H = −5.4279 × 10⁻¹³, I = 2.1107 × 10⁻¹⁴ variation of airspaces for magnification change f 32.31 62.52 121.27 D₁ 1.308 9.163 16.353 D₂ 2.137 7.795 13.105 D₃ 15.112 7.230 1.801 D₄ 6.458 27.256 63.798

ΣD₄/y=0.09, (r_(F)+r_(R))/(r_(F)−r_(R))=−1.05, ν_(R)=55.53, β_(4T)/β_(4W)=3.09, f_(BW)/f_(W)=0.20, f₄/f_(W)=0.62, β_(3T)=0.63, y/f₁=0.017, |f₄|/y=0.92, E(W)/f_(W)=0.25, |f_(T)/f₁|=0.097

Embodiment 18 f = 39.15˜67.51˜116.43, F number = 4.64˜7.08˜10.82 2ω = 57.0°˜35.0°˜21.0° r₁ = −44.3760 d₁ = 1.8000 n₁ = 1.78472 ν₁ = 25.68 r₂ = −1897.3346 d₂ = 0.1500 r₃ = 22.6448 d₃ = 2.3000 n₂ = 1.51823 ν₂ = 58.90 r₄ = 128.2210 d₄ = D₁ (variable) r₅ = 25.7558 d₅ = 2.1000 n₃ = 1.67270 ν₃ = 32.10 r₆ = 109.3944 d₆ = 1.5000 r₇ = ∞ (stop) d₇ = D₂ (variable) r₈ = −15.5145 d₈ = 1.6000 n₄ = 1.78472 ν₄ = 25.68 r₉ = −23.2694 d₉ = 3.2938 r₁₀ = 156.6330 d₁₀ = 3.8000 n₅ = 1.52542 ν₅ = 55.78 r₁₁ = −17.0510 (aspherical surface) d₁₁ = D₃ (variable) r₁₂ = −14.7576 (aspherical surface) d₁₂ = 1.9000 n₆ = 1.52542 ν₆ = 55.78 r₁₃ = 98.3688 d₁₃ = D₄ (variable) r₁₄ = ∞ (image) aspherical surface coefficients (11th surface) K = 0.5464, E = 7.1858 × 10⁻⁵, F = 2.5263 × 10⁻⁷, G = −5.2903 × 10⁻¹¹, H = 1.2826 × 10⁻¹¹ (12th surface) K = −1.1783, E = 1.7880 × 10⁻⁵, F = 1.4896 × 10⁻⁷, G = 1.5120 × 10⁻⁹, H = 3.5627 × 10⁻¹² f 39.15 67.51 116.43 variation of airspaces for magnification change D₁ 2.000 5.221 9.837 D₂ 3.043 6.685 9.003 D₃ 14.952 7.063 2.000 D₄ 9.737 31.744 68.918 variation of airspaces for focusing D₁ 0.640 3.645 8.000 D₂ 3.043 6.685 9.003 D₃ 16.312 8.639 3.838 D₄ 9.737 31.744 68.918

ΣD₄/y=0.09, (r_(F)+r_(R))/(r_(F)−r_(R))=−0.74, ν_(R)=55.78, β_(4T)/β_(4W)=2.69, f_(BW)/f_(W)=0.25, f₄/f_(W)=0.62, β_(3T)=0.66, y/f₁=0.043, |f₄|/y=1.12, E(W)/f_(W)=0.19, |f_(T)/f₁=0.233

Embodiment 19 f = 32.33˜62.05˜121.25, F number = 4.60˜6.85˜10.20 2ω = 66.0°˜37.6°˜20.0° r₁ = −39.6039 d₁ = 1.8754 n₁ = 1.84666 ν₁ = 23.78 r₂ = −276.2516 d₂ = 1.5832 r₃ = 109.0209 d₃ = 3.1462 n₂ = 1.48749 ν₂ = 70.23 r₄ = −36.6668 d₄ = D₁ (variable) r₅ = 14.6902 d₅ = 2.1417 n₃ = 1.75520 ν₃ = 27.51 r₆ = 23.7300 d₆ = D₂ (variable) r₇ = ∞ (stop) d₇ = D₃ (variable) r₈ = −13.9665 d₈ = 1.8384 n₄ = 1.80518 ν₄ = 25.42 r₉ = −23.0892 d₉ = 1.7116 r₁₀ = 45.6985 d₁₀ = 4.1799 n₅ = 1.51633 ν₅ = 64.14 r₁₁ = −14.7122 (aspherical surface) d₁₁ = D₄ (variable) r₁₂ = −13.8395 (aspherical surface) d₁₂ = 2.4679 n₆ = 1.72000 ν₆ = 41.99 r₁₃ = −14.7333 d₁₃ = 1.7331 n₇ = 1.81600 ν₇ = 46.62 r₁₄ = −221.8476 d₁₄ = D₅ (variable) r₁₅ = ∞ (image) aspherical surface coefficients (11th surface) K = −0.0572, E = 8.7137 × 10⁻⁵, F = −9.2710 × 10⁻⁸, G = 9.3414 × 10⁻⁹, H = −1.6728 × 10⁻¹¹, I = −7.8891 × 10⁻¹³ (12th surface) K = −0.1666, E = 4.9107 × 10⁻⁵, F = 4.4851 × 10⁻⁸, G = 4.3985 × 10⁻¹¹, H = 4.4643 × 10⁻¹², I = −3.4192 × 10⁻¹⁴ variation of airspaces for magnification change f 32.33 62.05 121.25 D₁ 1.206 9.792 18.510 D₂ 2.030 3.506 6.878 D₃ 3.029 5.933 7.283 D₄ 13.201 6.475 1.723 D₅ 6.177 26.818 63.812

ΣD₄/y=0.19, (r_(F)+r_(R))/(r_(F)−r_(R))=−1.13, ν_(R)=46.62(x), β_(4T)/β_(4W)=3.15, f_(BW)/f_(W)=0.19, f₄/f_(W)=0.56, β_(3T)=0.62, y/f₁=0.017, |f₄|/y=0.84, E(W)/f_(W)=0.27, |f_(T)/f₁|=0.097

wherein the reference symbol r₁, r₂, . . . represent radii of curvature on surfaces of respective lens elements, the reference symbols d₁, d₂, . . . designate distances between surfaces, the reference symbols n₁, n₂, . . . denote refractive indices of the lens elements, and the reference symbols ν₁, ν₂, . . . represent Abbe's numbers of the respective lens elements.

The first embodiment is composed, as shown in FIG. 4, of a first lens unit G1 which is composed of a negative lens element L1 and a positive lens element L2, a second lens unit G2 which is composed of a positive lens element L3 and an aperture stop S, a third lens unit G3 which is composed of a negative lens element L4 and a positive lens element L5, and a fourth lens unit G4 which is composed of a negative lens element L6: the first embodiment being composed of six lens element in total. The first embodiment is configured to change its magnification from a wide position to a tele position by moving all the lens units toward the object side so as to widen an airspace reserved between the second lens unit G2 and the third lens unit G3. Further, the first lens unit G1 and the fourth lens unit G4 are moved as an integral unit, thereby making it possible to reduce a number of zooming cams and simplify a structure of a lens barrel. Furthermore, the first embodiment is focused by moving the third lens unit G3.

In the first embodiment, aspherical surfaces are used on the fifth lens element L5 which is disposed on the image side in the third lens unit G3 and the sixth lens element L6 which is used as the fourth lens unit.

Further, the fifth lens element LS and the sixth lens element L6 are made of a plastic material. The plastic material is selected for lowering manufacturing costs of the aspherical lens elements. The plastic lens elements are configured as the positive lens element and the negative lens element so that variations due to temperature and humidity changes are produced in directions reverse to each other, whereby the zoom optical system as a whole is scarcely influenced by the variations.

FIG. 4 shows the zoom optical system at a wide position (W), at an intermediate focal length (S), at a tele position (T) and in a collapsed condition (C) in a sequence from the uppermost stage.

The second embodiment has a composition illustrated in FIG. 5, or remains unchanged from the first embodiment in its composition and movements of lens units for a magnification change, but uses a fifth lens element LS and a sixth lens element L6 which are configured as aspherical lens elements made of a glass material. Accordingly, the second embodiment is free from influences due to temperature and humidity changes.

Since a third lens unit G3 has a magnification of approximately 1× within an entire zooming region in the second embodiment, the third lens unit G3 must be moved for a long distance when the second embodiment is focused by moving only the third lens unit G3. It is therefore preferable to focus the second embodiment by moving a second lens unit G2 and the third lens unit G3 as an integral unit or moving a fourth lens unit G4.

Like FIG. 4, FIG. 5 shows the zoom optical system at a wide position (W), at an intermediate focal length, at a tele position (T) and in a collapsed condition (C) in a sequence from the uppermost stages.

The third embodiment remains unchanged from the second embodiment in its composition, but lens units are moved for a magnification change so that an airspace reserved between a second lens unit and a third lens unit is minimum at an intermediate focal length. Further, an aspherical surface is used on each of second, third and fourth lens units G2, G3 and G4. The third embodiment is focused by moving the third lens unit G3 toward the object side.

The fourth embodiment has a composition illustrated in FIG. 7, or is composed of a first lens unit G1 which is composed of a negative lens element L1 and a positive lens element L2, a second lens unit G2 which is composed of an aperture stop S, a negative lens element L3 and a positive lens element L4, a third lens unit G3 which is composed of a negative lens element L5 and a positive lens element L6, and a fourth lens unit G4 which is composed of a negative lens element L7, and configured to change its magnification from a wide position to a tele position by moving the lens units toward the object side so as to narrow an airspace reserved between the second lens unit G2 and the third lens unit G3. An aspherical surface is used on each of the second lens unit G2 and the fourth lens unit G4.

The fourth embodiment is focused by moving the fourth lens unit G4 toward the image side.

The fifth embodiment has a composition illustrated in FIG. 8, or is composed of a first lens unit G1 which is composed of a negative lens element L1 and a positive lens element L2, a second lens unit G2 which is composed of an aperture stop S and a positive lens element L3, a third lens unit G3 which is composed of a positive lens element L4, a negative lens element L5 and a positive lens element L6, and a fourth lens unit G4 which is composed of a negative lens element L7, and configured to change its magnification by moving the lens units toward the object side so as to widen an airspace reserved between the second lens unit G2 and the third lens unit G3. The fifth embodiment uses an aspherical surface on each of the third lens unit G3 and the fourth lens unit G4.

The fifth embodiment is focused by moving the third lens unit G3 toward the object side.

The sixth embodiment has a composition illustrated in FIG. 9, or is composed of a first lens unit G1 which is composed of a positive lens element L1 and a negative lens element L2, a second lens unit G2 which is composed of a positive lens element L3, a third lens unit G3 which is composed of a negative lens element L4, a positive lens element L5 and an aperture stop S disposed between these lens elements, and a fourth lens unit G4 which is composed of a negative lens element L6 having an aspherical resin layer (a layer which is formed between an aspherical surface r₁₁ and a surface r₁₂, and has thickness d₁₁), and configured to change its magnification by moving the lens units so as to narrow an airspace reserved between the second lens unit G2 and the third lens unit G3. An aspherical surface is used on each of the third lens unit G3 and the fourth lens unit G4.

The sixth embodiment is focused by moving the second lens unit G2 and the third lens unit G3 as an integral unit or the fourth lens unit only.

The seventh embodiment is an optical system which has a composition illustrated in FIG. 10, or is composed of a first lens unit G1 which is composed of a positive lens element L1, a second lens unit G2 which is composed of a positive lens element L2, a third lens unit G3 which is composed of an aperture stop S, a negative lens element L3 and a positive lens element L4, a fourth lens unit G4 which is composed of a negative lens element L5 having an aspherical resin layer (a layer which is formed between an aspherical surface r₁₀ and a surface r₁₁, and has thickness d₁₀), and configured to change its magnification by moving the lens units toward the object side so as to minimize an airspace reserved between the second lens unit G2 and the third lens unit G3 at an intermediate focal length. The second lens unit G2 and the fourth lens unit G4 are moved as an integral unit for changing the magnification so that a number of zooming cams can be reduced and a structure of a lens barrel can be simplified.

The seventh embodiment is focused by moving the second lens unit G2 and the third lens unit as an integral unit or the fourth lens unit G4 only.

The seventh embodiment uses an aspherical surface on each of the lens units. It is possible to further enhance optical performance of the seventh embodiment by increasing the number of the aspherical surfaces, or adopting an aspherical lens element which has aspherical surfaces on both sides. In addition, it is possible also in the second through fifth embodiments to configure the plastic aspherical lens elements as hybrid lens elements having aspherical resin layers such as those used in the sixth and seventh embodiments.

The eighth embodiment has a composition illustrated in FIG. 11, or is composed of a first lens unit G1 which is composed of a negative lens element L1 and a positive lens element L2, a second lens unit G2 which is composed of a positive lens element L3 and an aperture stop S, a third lens unit G3 which is composed of a negative lens element L4 and a positive lens element L5, and a fourth lens unit G4 which is composed of a negative lens element L6, and configured to change its magnification from a wide position to a tele position by moving the lens units toward the object side so as to widen an airspace reserved between the second lens unit G2 and the third lens unit G3.

The eighth embodiment is focused by moving the third lens unit G3 toward the object side.

The eighth embodiment uses an aspherical surface on each of the fifth and sixth lens elements L5 and L6 which are disposed in the third lens unit G3 and the fourth lens unit G4. The fifth and sixth lens elements are made of a plastic material for lowering a manufacturing cost. When the fifth positive lens element L5 and the sixth negative lens element L6 are made of a plastic material, these lens elements are varied reversely by temperature and humidity changes, whereby influences due to temperature and humidity changes are reduced in the zoom optical system as a whole.

In each of the embodiments described above, the fourth lens unit G4 is composed of a single negative lens element which has a deep concave surface on the object side so that the zoom optical system is compact in its collapsed condition.

The ninth embodiment is a zoom optical system which has a field angle 2ω of 65° or wider in a wide angle region and a vari-focal ratio on the order of 3.8.

The ninth embodiment has a composition illustrated in FIG. 12, or is composed of a first lens unit G1 which is composed of a negative lens element L1 and a positive lens element L2, a second lens unit G2 which is composed of a positive lens element L3 and an aperture stop S, a third lens unit G3 which is composed of a negative lens element L4 and a positive lens element L5, and a fourth lens unit G4 which is composed of a negative lens element L6. That is, the zoom optical system preferred as the ninth embodiment as a whole composed of six lens elements.

The ninth embodiment is configured to change its magnification from a wide position to a tele position by moving the lens units toward the object side so as to widen an airspace reserved between the second lens unit and the third lens unit. The ninth embodiment is focused by moving the third lens unit G3 toward the object side.

The ninth embodiment uses an aspherical surface on each of the positive lens element L5 disposed in the third lens unit and the negative lens element L6 disposed in the fourth lens unit.

The ninth embodiment allows aberrations to be varied extremely little when it is focused on an object located at a short distance by moving the third lens unit G3.

The tenth embodiment is a zoom optical system which has a field angle 2ω of 65° or wider in a wide angle region and a vari-focal ratio on the order of 3.8.

The tenth embodiment has a composition illustrated in FIG. 13, or is composed of a first lens unit G1 which is composed of a negative lens element L1 and a positive lens element L2, a second lens unit G2 which is composed of a positive lens element L3, a third lens unit G3 which is composed of a negative lens element L4, a positive lens element L5 and a positive lens'element L6, and a fourth lens unit G4 which is composed of a negative lens element L7. That is, the zoom optical system preferred as the tenth embodiment as a whole is composed of seven lens elements.

The tenth embodiment is also configured to change its magnification from a wide position to a tele position by moving the lens units toward the object side so as to widen an airspace reserved between the second lens unit and the third lens unit. The tenth embodiment is focused by moving the third lens unit toward the object side.

The tenth embodiment uses an aspherical surface on each of the positive lens element disposed on the image side in the third lens unit G3 and the negative lens element disposed in the fourth lens unit G4.

The eleventh embodiment is a zoom optical system which has a composition illustrated in FIG. 14, a field angle 2ω of 70° or wider in a wide angle region and a vari-focal ratio on the order of 3.8.

The eleventh embodiment is a zoom optical system which is composed of four lens units of six lens elements as shown in FIG. 14 or similarly to the ninth embodiment.

The twelfth embodiment is a zoom optical system which has a composition illustrated in FIG. 15, a field angle 2ω of 70° or wider in a wide angle region and a vari-focal ratio on the order of 4.2.

The twelfth embodiment is also a zoom optical system which has a composition similar to that of the ninth embodiment.

The thirteenth embodiment is a zoom optical system which has a composition illustrated in FIG. 16, a field angle 2ω of 65° or wider in a wide angle region and a vari-focal ratio on the order of 4.7.

The thirteenth embodiment is also an optical system which has a composition similar to that of the ninth embodiment.

The fourteenth embodiment is a zoom optical system which has a composition illustrated in FIG. 17 and a field angle 2ω of 65° in a wide angle region, or wider and a vari-focal ratio on the order of 3.7.

The optical system preferred as the fourteenth embodiment also has a composition which is similar to that of the ninth embodiment.

A negative lens element used as a fourth lens unit of the fourteenth embodiment is configured as a hybrid lens element which has an aspherical resin layer on an object side surface thereof.

The fifteenth embodiment has a composition illustrated in FIG. 18, or is composed, in order from the object side, of a first lens unit G1 which is composed of a negative lens element L1 and a positive lens element L2, and has a positive power, a second lens unit G2 which is composed of a positive lens element L3 and a stop, and has a positive power, a third lens unit G3 which is composed of a negative lens element L4 and a positive lens element L5, and has a positive power, and a fourth lens unit G4 which is composed of a negative lens element L5 and has a negative power: the fifteenth embodiment as a whole being composed of six lens elements. The optical system preferred as the fifteenth embodiment is configured to change its magnification from a wide position to a tele position by moving all the lens units toward the object side so as to widen an airspace reserved between the second lens unit and the third lens unit.

The fifteenth embodiment uses an aspherical surface on each of the positive lens element L5 disposed in the third lens unit G3 and the negative lens element L6 disposed in the fourth lens unit G4. The aspherical lens element L5 disposed in the third lens unit G3 and the aspherical lens element L6 disposed in the fourth lens unit are made of a plastic material for lowering a manufacturing cost of the zoom optical system. Further, variations due to temperature and humidity changes are cancelled with each other since the positive lens element and the negative lens element are made of the plastic material.

The sixteenth embodiment has a composition illustrated in FIG. 19, or remains unchanged from the fifteenth embodiment in composition and movements of lens units for changing a magnification. The sixteenth embodiment is focused by moving a second lens unit and a third lens unit toward the object side.

The seventeenth embodiment has a composition illustrated in FIG. 20, or remains unchanged from the fifteenth embodiment in composition and movements of lens unit for changing a magnification. In the seventeenth embodiment, however, a positive lens element L5 disposed in a third lens unit G3 and a negative lens element L6 disposed in a fourth lens unit G4 are aspherical lens elements which are made of a glass material. Accordingly, the seventeenth embodiment is free from influences due to temperature and humidity changes. Further, the negative lens element L6 disposed in the fourth lens unit G4 can be configured as a hybrid lens element which has an aspherical resin layer.

The eighteenth embodiment has a composition illustrated in FIG. 21, or remains unchanged from the fifteenth embodiment in composition and movements of lens units for a magnification change.

The eighteenth embodiment is focused on an object located at a short distance by moving a second lens unit and a third lens unit toward the object side.

The nineteenth embodiment is composed, in order from the object side as shown in FIG. 22, of a first positive lens unit G1 which is composed of a negative lens element Ll and a positive lens element L2, a second positive lens unit G2 is composed of a positive lens element L3, a third positive lens unit G3 which is composed of a negative lens element L4 and a positive lens element L5, and a fourth negative lens unit G4 which is composed of a cemented lens component consisting of a positive meniscus lens element L6 and a negative lens element L7, and configured to change its magnification from a wide position to a tele position by moving the lens units so as to widen an airspace reserved between the second lens unit and the third lens unit. That is, the nineteenth embodiment as a whole is composed of seven lens elements.

Further, an aperture stop is disposed between the second lens unit and the third lens unit, and moved so as to widen an airspace reserved between the second lens unit and the aperture stop for changing a magnification from the wide position to the tele position. Furthermore, an aspherical surface is used in each of the third lens unit and the fourth lens unit.

The aspherical surfaces used in the embodiments described above have shapes which are expressed by the formula shown below:

x=(y ² /r)/[1+{1−(1+k)(y/r)²}^(1/2) ]+Ey ⁴ +Fy ⁶ +Gy ⁸⁺ Hy ¹⁰ +IY ¹²

wherein a direction of an optical axis is taken as x, a direction perpendicular to the optical axis is taken as y, the reference symbol k represents a conical constant, and the reference symbols E, F, G, H, I, . . . designate aspherical surface coefficients of the fourth, sixth, eighth, tenth, twelfth orders respectively. 

What is claimed is:
 1. A zoom optical system comprising: a front lens group which comprises a plurality of lens units and has a positive power, wherein all the lens units in the front lens group are movable; and a rear lens group which has a negative power, wherein at least one negative lens component disposed in said rear lens group is a cemented lens component consisting of an aspherical glass lens element having a meniscus shape and a spherical lens element.
 2. A zoom optical system comprising: a front lens group which comprises plurality of lens units and has a positive power, wherein all the lens units in the front lens group are movable; and a rear lens group which has a negative power, wherein at least one lens component disposed in said rear lens group is a cemented lens component consisting of an aspherical glass lens element having a meniscus shape and a spherical lens element, and said plurality of lens units are moved so as to change airspaces among said lens units for changing a magnification of said zoom optical system.
 3. A-zoom optical system comprising: a first lens group which comprises a plurality of lens units and has a positive power, wherein all the lens units in the first lens group are movable; and a second lens group which has a negative power, wherein at least one negative lens component disposed in said second lens group is a cemented lens component consisting of an aspherical glass lens element having a meniscus shape and a spherical lens element.
 4. The zoom optical system according to claim 1 or 2, wherein said plurality of lens unit in the front lens group comprises, in order from the object side, a first lens unit, a second lens unit and a third lens unit, wherein said rear lens group consists of a fourth lens unit and wherein said first, second and third lens units are movable to change a magnification.
 5. The zoom optical system according to claim 4 satisfying the following condition (1): 0.03<ΣD ₄ /y<0.25  (1) wherein the reference symbol ΣD4 represents a structural length of the fourth lens unit and the reference symbol y designates ½ of a diagonal length of an image surface.
 6. The zoom optical system according to claim 4 satisfying the following condition (2): −1.2<(r _(F) +r _(R))/(r _(F) −r _(R))<0  (2) wherein the reference symbols rF and rR represent radii of curvature on an object side surface and an image side surface respectively of the fourth lens unit.
 7. The zoom optical system according to claim 4 satisfying the following condition (4-1): 1.5<β_(4T)/β_(4W)<6.0  (4-1) wherein the reference symbols β_(4T) and β_(4W) represent lateral magnifications of the fourth lens unit at a tele position and a wide position respectively.
 8. The zoom optical system according to claim 4 satisfying the following condition (8): 0≦y/f ₁≦0.14  (8) wherein the reference symbol y represents ½ of a diagonal length of an image surface and the reference symbol f1 designates a focal length of the first lens unit.
 9. The zoom optical system according to claim 4 satisfying the following condition (6): 0.5<|f ₄ /f _(W)|<0.9  (6) wherein the reference symbol f4 represents a focal length of the fourth lens unit and the reference symbol fW designates a focal length of the optical system as a whole at a wide position.
 10. The zoom optical system according to claim 4 satisfying the following condition (3): ν_(R)>50  (3) wherein the reference symbol νR represents an Abbe's number of the negative lens element disposed in the fourth lens unit.
 11. The zoom optical system according to claim 4 satisfying the following condition (7): |β_(3T)|<0.9  (7) wherein the reference symbol β3T represents a lateral magnification of the third lens unit at a tele position.
 12. The zoom optical system according to claim 4 satisfying the following condition (11): |f _(T) /f ₁|≦0.6  (11) wherein the reference symbol f1 represents a focal length of the first lens unit and the reference symbol fT designates a focal length of the optical system as a whole at a tele position.
 13. The zoom optical system according to claim 1 or 2, wherein said plurality of lens units in the front lens group comprises, in order from the object side, a first lens unit and a second lens unit, and wherein said first lens unit and said second lens unit are moved to change a magnification.
 14. The zoom optical system according to claim 13 satisfying the following condition (8): 0≦y/f ₁≦0.14  (8) wherein the reference symbol y represents ½ of a diagonal length of an image surface and the reference symbol f1 designates a focal length of the first lens unit.
 15. The zoom optical system according to claim 13 satisfying the following condition (11): |f _(T) /f ₁|≦0.6  (11) wherein the reference symbol f₁ represents a focal length of the first lens unit and the reference symbol f_(T) designates a focal length of the optical system as a whole at a tele position.
 16. The zoom optical system according to claim 1 or 2, wherein said plurality of lens units in the front lens group comprises a first lens unit disposed on the most object side and satisfying the following conditions (8): 0≦y/f ₁≦0.14  (8) wherein the reference symbol y represents ½ of a diagonal length of an image surface and the reference symbol f₁ designates a focal length of the first lens unit.
 17. The zoom optical system according to claim 1 or 2, wherein said plurality of lens units in the front lens group comprises a first lens unit disposed on the most object side and satisfying the following condition (11): |f _(T) /f ₁|≦0.6  (11) wherein the reference symbol f₁ represents a focal length of the first lens unit and the reference symbol f_(T) designates a focal length of the optical system as a whole at a tele position.
 18. The zoom optical system according to claim 1, 2 or 3 satisfying the following condition (10): 0.10≦E(W)/f _(W)≦0.30  (10) wherein the reference symbol E(W) represents a distance as measured from a vertex of a first lens surface to an entrance pupil of the optical system along an optical axis in a wide position and the reference symbol f_(W) designates a focal length of the optical system as a whole in the wide position.
 19. The zoom optical system according to claim 1, 2 or 3 satisfying the following condition (5): 0.1<f _(BW) /f _(W)<0.5  (5) wherein the reference symbol fBW represents a back focal length at a wide position and the reference symbol fW designates a focal length of the optical system as a whole at the wide position.
 20. The zoom optical system according to claim 1, 2 or 3, wherein said aspherical glass lens element has a smooth surface which is kept in contact with air and a rough surface which is cemented to said spherical lens element.
 21. A zoom optical system comprising: a front lens group which comprises a plurality of movable lens units and has a positive power, and a rear lens group which has a negative power, wherein at least one lens component disposed in said zoom optical system is a cemented lens component consisting of an aspherical glass lens element having a meniscus shape and a spherical lens element, and said aspherical glass lens element has a smooth surface which is kept in contact with air and a rough surface which is cemented to said spherical lens element.
 22. A zoom optical system comprising: a front lens group which comprises, in order from the object side, a first lens unit, a second lens unit and a third lens unit and has a positive power, wherein all the lens units in the front lens group are movable; and a rear lens group which consists of a fourth lens unit and has a negative power, wherein at least one lens component disposed in said zoom optical system is a cemented lens component consisting of an aspherical glass lens element having a miniscus shape and a spherical lens element, and wherein said first, second and third lens units are movable to change a magnification and wherein said fourth lens unit satisfies the following conditions (1): 0.03<ΣD ₄ /y<0.25  (1) wherein the reference symbol ΣD₄ represents a structural length of the fourth lens unit and the reference symbol y designates ½ of a diagonal length of an image surface.
 23. A zoom optical system comprising: a front lens group which comprises a plurality of lens units and has a positive power, wherein all the lens units in the front lens group are movable; and a rear lens group which has a negative power, wherein at least one lens component disposed in said zoom optical system is a cemented lens component consisting of an aspherical glass lens element having a meniscus shape and a spherical lens element, wherein said zoom lens optical system satisfies the following condition (10): 0.10≦E(W)/f _(W)≦0.30  (10) wherein the reference symbol E(W) represents a distance as measured from a vertex of a first lens surface to an entrance pupil of the optical system along an optical axis in a wide position and the reference symbol f_(W) designates a focal length of the optical system as a whole at the wide position.
 24. A zoom optical system comprising: a front lens group which comprises, in order from the object side, a first lens unit, a second lens unit and a third lens unit and has a positive power, wherein all the lens units in the front lens group are movable; and a rear lens group which consists of a fourth lens unit and has a negative power, wherein at least one lens component disposed in said zoom optical system is a cemented lens component consisting of an aspherical glass element having a meniscus shape and aspherical lens element and wherein said first, second and third lens units are movable to change a magnification and wherein said fourth lens unit satisfies the following condition (4-1): 1.5<β_(4T)/β_(4W)<6.0  (4-1) wherein the reference symbols β_(4T) and β_(4W) represent lateral magnifications of the fourth lens unit at a tele position and a wide position respectively.
 25. A zoom optical system comprising: a front lens group which comprises, in order from the object side, a first lens unit, a second lens unit and a third lens unit and has a positive power, wherein all the lens units in the front lens group are movable; and a rear lens group which consists of a fourth lens unit and has a negative power, wherein at least one lens component disposed in said zoom optical system is a cemented lens component consisting of an aspherical glass lens element having a meniscus shape and a spherical lens element, and wherein said first, second and third lens units are movable to change a magnification and wherein said third lens unit satisfies the following condition (7): |β_(3T)|<0.9  (7) wherein the reference symbol β3T represents a lateral magnification of the third lens unit at tele position.
 26. A zoom optical system comprising: a front lens group which comprises a plurality of lens units and has a positive power, wherein all the lens units in the front lens group are movable; and a rear lens group which has a negative power, wherein at least one lens component disposed in said zoom optical system is a cemented lens component consisting of an aspherical glass lens element having a meniscus shape and a spherical lens element, wherein said plurality of lens units in the front lens group comprises a first lens unit disposed on the most object side and satisfies the following condition (8): 0≦y/f ₁≦0.14  (8) wherein the reference symbol y represents ½ of a diagonal length of an image surface and the reference symbol f₁ designates a focal length of the first lens unit.
 27. A zoom optical system comprising: a front lens group which comprises a plurality of lens units and has a positive power, wherein all the lens units in the front lens group are movable; and a rear lens group which has a negative power, wherein at least one lens component disposed in said zoom optical system is a cemented lens component consisting of an aspherical glass lens element having a meniscus shape and a spherical lens element, wherein said plurality of lens units in the front lens group comprises a first lens unit disposed on the most object side and satisfies the following condition (11):  |f _(T) /f ₁|≦0.6  (11) wherein the reference symbol f₁ represents a focal length of the first lens unit and the reference symbol f_(T) designates a focal length of the optical system as a whole at a tele position.
 28. A zoom optical system comprising: a first lens group which has a positive power; and second lens group which has a negative power, wherein said zoom optical system comprises a plurality of lens units and all the lens units in the zoom optical system are movable, and wherein at least one negative lens component disposed in said second lens group is a cemented lens component consisting of an aspherical glass lens element having a meniscus shape and a spherical lens element. 